This commit is contained in:
fmq
2026-07-21 22:25:14 +08:00
parent 15971a5e01
commit c53fc99c1d
298 changed files with 459694 additions and 31 deletions
+268
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PRO conv_spec,sx,sy,px,py,cx,cy
; note
; no zero padding applied, however sufficient precision also at end points
; note also, that response function centered, not wrapped arround,
; since referred to central frequency of signal.
n = n_elements(sx)
if n ne n_elements(px) then print,'error: different array dimensions'
shft = long(n/2)
tty = fltarr(n) + (sy(0)+sy(n-1))/2.
sy_t = sy - tty
cx = sx
cy = shift(fft(fft(sy_t,-1)*fft(py,-1),1),shft)
cy = ((cx(n-1)-cx(0))/(n-1)) * n * cy ; renormalise result of convolution
cy = cy + tty
END
PRO convol,sx,sy,cx,cy,vdop=vdop,fwhm=fwhm,resol=resol,vsini=vrot,beta=beta,vmacro=vmacro,message=message,original=original,help=help
if n_params() lt 4 then begin
print,'PRO convol,sx,sy,cx,cy[,vdop=[Km/s],fwhm=,resol=,vsini=[Km/s],beta=,vmacro=[Km/s],/message,/original]'
if keyword_set(help) then begin
; written by J. Puls, modified by J. Sundqvist
; spectrum is convolved as specified with keywords. units in
; Aangstrom or km/s.
print,'input'
print,'; sx : wavelength vector'
print,'; sy : flux vector'
print,'; cx : wavelength vector after convolution'
print,'; cy : flux vector after convolution'
;
print,'; keywords'
print,'; vdop : doppler width [km/s]'
print,'; fwhm : fwhm of gaussian profile [AA] '
print,'; resol : resolution=lambda0/fwhm'
print,'; vsini : projected rotational velocity [km/s]'
print,'; beta : constant used for rotation'
print,'; vmacro : radial-tangential macroturbulence'
print,'; (v_radial=v_tangential) [km/s]'
print,'; message : some information is printed'
print,'; original : if set, remap finally onto original'
print,'; wavelength grid. OBS:linear interpolation.'
;
print,'; note:'
print,'; keywords fwhm, resol, vdop mutually exclusive.'
print,'; if more than one set, the last is ignored'
print,'; if vsini set, rotational folding is done first'
endif
return
endif
;maximum resolution
max_resol=2d5
;max_resol=3d4
;default settings
if not keyword_set(beta) then beta = 1.5
if not keyword_set(message) then message = 0
if not keyword_set(original) then original = 0
if not keyword_set(vrot) then vrot = 0.d
;constants
clight = 299792.5d
rsmpl_fac = 0.7d
;wavelength vector must be strictly increasing!
i=sort(sx)-lindgen(n_elements(sx))
if max(i) ne 0 then begin
print,'Wavelength vector must be strictly increasing - sort!'
print,'returning'
return
endif
sxx = sx
syy = sy
n = n_elements(sxx)
nn = n
rdst= (sxx(n-1)-sxx(0))/double(n-1) ; resampling distance
intp= 0
;check if wavelength vector equidistant
dsx = abs(sxx(1:*)-sxx(0:n-2))
rdst_min = min(dsx,max=rdst_max)
meanw = 0.5d*(sxx(0)+sxx(n-1))
eps = meanw/max_resol
diff = abs(rdst_max-rdst_min)
not_eqdist = diff gt eps
if not_eqdist then begin
if message then print,'spectrum is not equidistant: rdmin= ',rdst_min,', rdmax= ',rdst_max
rdst = MAX([(rdst_min * rsmpl_fac),eps])
intp = 1
nn = (sxx(n-1)-sxx(0))/rdst
endif
xpow = alog(nn)/alog(2.)
pow = long(xpow)
if ((pow le 14 and pow gt 2) or intp) and ((xpow-pow) ne 0.) then begin
pow = pow + 1
nn_x = long(2.^pow)
if (float(nn)/float(nn_x) gt rsmpl_fac) and (not not_eqdist) then begin
nn = nn_x * 2l
endif else begin
nn = nn_x
endelse
rdst = (sxx(n-1)-sxx(0))/(nn-1)
sxx = lindgen(nn)*rdst + sx(0)
syy = interpol(sy,sx,sxx,/spline)
res=finite(syy)
bres=where(res eq 0, countb)
if countb ne 0 then begin
for i=0,nn-1 do begin
b=where(sx eq sxx(i),count)
if count gt 1 then begin
sym=mean(sy(b))
syy(i)=sym
endif
endfor
endif
if message then begin
print,'resampled grid with resampling distance: ',rdst
print, nn, format= "('resampled spectrum has ',i6,' points')"
endif
endif
px = (findgen(nn)-long(nn/2))*rdst
;rotation
if keyword_set(vrot) and vrot ge 0.1 then begin
lambda0 = (sxx(nn-1)+sxx(0))/2.
dlam_max = vrot*(lambda0/clight)
xx = px / dlam_max
one = where(abs(xx) gt 1)
xx(one) = 1.
xx_2 = xx*xx
unsoeld = (2.* sqrt(1-xx_2)/!pi + (1-xx_2)*beta/2.) / (1 + 2*beta/3.)
; gray = (2.*(1-beta)*sqrt(1-xx_2)/!pi + (1-xx_2)*beta/2.) / (1 - beta/3.)
py = unsoeld
py = py / dlam_max
conv_spec,sxx,syy,px,py,cx,cy
sxx = cx
syy = cy
endif
;macroturbulence
if keyword_set(vmacro) then begin
aar=1.
spi=sqrt(!dpi)
lambda0 = (sxx(nn-1) + sxx(0))/2.
mr=(vmacro*lambda0/clight)[0]
ccr=2.*aar/spi/mr
pxmr=abs(px)/mr
py=ccr*[exp(-pxmr^2)+spi*pxmr*(errorf(pxmr)-1.)]
py=py/int_tabulated(px,py,/double); to be sure the distribution is normalized
conv_spec,sxx,syy,px,py,cx,cy
sxx = cx
syy = cy
endif
;Gauss profile
if keyword_set(vdop) or keyword_set(fwhm) or keyword_set(resol) then begin
fac = 2.*sqrt(alog(2.))
lambda0 = (sxx(nn-1)+sxx(0))/2.
if keyword_set(fwhm) then begin
dlam_dop = fwhm/fac
vdop = dlam_dop*clight/lambda0
endif else if keyword_set(resol) then begin
vdop=clight/(resol*fac)
dlam_dop = vdop*(lambda0/clight)
endif else begin
dlam_dop = vdop*(lambda0/clight)
endelse
min_cnr = 5
max_cnr = long(nn*0.8)
if message then begin
print, vdop, dlam_dop, format="('vdop=',f7.3,'km/s <=>',f7.3,'a')"
print,fac*vdop,fac*dlam_dop, format="('fwhm=',f7.3,'km/s <=>',f7.3,'a')"
endif
cnr = long(4.*dlam_dop/rdst) + 1
if max_cnr le cnr then begin
percent = cnr/float(nn)*100.
print,'gauss profile is very large:' + string(percent,'(f6.2)') $
+ '% of spectrum points are forming the profile'
endif
if min_cnr ge cnr then begin
print,'gauss profile is very small: only ' + string(cnr,'(i4)') $
+ ' data points are forming the profile'
endif
xx = px / dlam_dop
six = where(abs(xx) lt 6.)
py = fltarr(nn)
py(six) = exp(-(xx(six)^2))/(sqrt(!pi)*dlam_dop)
conv_spec,sxx,syy,px,py,cx,cy
sxx = cx
syy = cy
endif
if original then begin
cy = interpol(syy,sxx,sx)
cx = sx
endif
;Return only real part
cy=real_part(cy)
cx=real_part(cx)
END
function fconvol,x,y,xout,rv=rv,vdop=vdop,fwhm=fwhm,resol=resol,vsini=vrot,beta=beta,vmacro=vmacro,message=message
xx=x[sort(x)]
yy=y[sort(x)]
yy=yy[uniq(xx)]
xx=xx[uniq(xx)]
n=n_elements(xx)
cc=2.99792458d5
if keyword_set(rv) then xx=xx*(1.0d - rv/cc)
if n_elements(xx) gt 50000 then begin
nps=25000l
segs=(n/nps)
yff=yy*0.0d
if n mod nps lt 1000 then begin
nps=24000l
segs=(n/nps)
endif
for ii=0, segs do begin
ind=[0l,nps-1l]+ii*nps
if (ii+1l)*nps gt n then ind[1]=n-1
cind=[max([0,ind[0]-1000l]), min([ind[1]+1000l,n-1])]
yff[ind[0] : ind[1]]=fconvol(xx[cind[0] : cind[1]],yy[cind[0] : cind[1]],xx[ind[0] : ind[1]],vdop=vdop,fwhm=fwhm,resol=resol,vsini=vrot,beta=beta,vmacro=vmacro,message=message)
endfor
yout=interpol(yff,xx,xout)
return,yout
endif
if odd(n_elements(xx)) then begin
xx=xx[1:*]
yy=yy[1:*]
endif
convol,xx,yy,nx,sol,vdop=vdop,fwhm=fwhm,resol=resol,vsini=vrot,beta=beta,vmacro=vmacro,message=message,/original
if n_elements(xout) gt 1 then yout=interpol(sol,xx,xout) else yout=sol
return,yout
end
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pro lineid_annot,wave,flux,wline,eqw,text1,text2,text3, $
charsize=charsize,extend=extend,charthick=charthick,_extra=pex
;+
; lineid_plot2b
;
; Plot spectrum with specified line identifications annotated at the
; top of the plot.
;
; CALLING SEQUENCE:
; lineid_annot,wave,flux,wline,eqw,text1,text2,text3, $
; charsize=charsize,extend = extend, charthick = charthick
;
; INPUTS:
; wave - wavelength vector for the plot
; flux - flux vector
; wline - vector of line identifications. (only the lines between
; the plot limits will be used)
; eqw - vector of equivalent widths
; text1 - string array of text to be used to annotate each line
; text2 - (OPTIONAL) second string array of text to be used for
; line annotation. Since the text is written with
; proportional spaced characters, TEXT2 can be used if
; you want two sets of annotation to be alinged:
;
; eg: Cr IV 1390.009
; Fe V 1390.049
; Ni IV 1390.184
; instead of
; Cr IV 1390.009
; Fe V 1390.049
; Ni IV 1390.184
; text3 - still additional text
;
; allows xyouts keywords
;
;
; OPTIONAL KEYWORD INPUTS:
;
; extend = specifies that the annotated lines should have a
; dotted line extended to the spectrum to indicate the
; line position. EXTEND can be a scalar (applies to
; all lines) or a vector with a different value for
; each line. The value of EXTEND gives the line
; IDL plot line thickness for the dotted lines.
; If EXTEND is a vector each dotted line can have a
; different thickness. A value of 0 indicates that
; no dotted line is to be drawn. (default = scalar 0)
; charsize = the character size of the annotation for each line.
; If can be a vector so that different lines are
; annotated with different size characters. Charsize
; can be used to make stronger lines have a larger
; annotation. (default = scalar 1.0).
; charthick = the character thickness of the annotation for
; each line. If can be a vector so that different lines
; are annotated with characters of varying thickness.
; CHARTHICK can be used to make stronger lines have
; a bolder annotation. (default = !p.charthick)
; OPERATIONAL NOTES:
;
; Once the program has completed, You can use OPLOT to draw additional
; plots on the display. The plots !X.TITLE and !Y.TITLE are used but
; the !P.TITLE (!MTITLE) is ignored.
;
; If your annotated characters are not being rotated properly,
; try setting !FANCY to a non zero value.
;
; !X.RANGE, !Y.RANGE or the routine SET_XY can be used to change
; plot limits before calling LINEID_PLOT.
;
; HISTORY:
; version 1 D. Lindler Jan, 1992
; Sept 27, 1993 DJL fixed bug in /extend option
; version 2 I. Hubeny Dec, 1993
; extension for selecting and plotting using equivalent width
;-
;----------------------------------------------------------------------------
if n_params(0) lt 1 then begin
print,'CALLING SEQUENCE: lineid_annot,wave,flux,wline,eqw,text1,[,text2,text3]'
print,'OPTIONAL KEYWORD PARAMETERS'
print,'EXTEND = switch for drawing indicating lines'
print,'CHARSIZE = character size'
print,'CHARTHICK = character thickness'
retall
end
;
; initialization
;
if n_elements(charsize) eq 0 then charsize=1
n = n_elements(wline)
if n_elements(text2) eq 0 then text2 = strarr(n)
if n_elements(text3) eq 0 then text3 = strarr(n)
if n_elements(charsize) eq 1 then csize = replicate(charsize,n) $
else csize = charsize
if n_elements(extend) eq 0 then extend = 0
if n_elements(extend) eq 1 then begin
if extend lt 0 then begin
ethick = alog10(eqw*abs(extend))
endif else ethick = replicate(extend,n)
endif else ethick = extend
if n_elements(charthick) eq 0 then cthick = !p.charthick $
else cthick = charthick
if n_elements(cthick) eq 1 then cthick = replicate(cthick,n)
;
; set plot area
;
; set_viewport,0.13,0.95,0.1,0.65
;
; plot data
;
; plot,wave,flux,title=' ',xstyle=1
;
; get data ranges
;
xmin = !x.crange(0)
xmax = !x.crange(1)
ymin = !y.crange(0)
ymax = !y.crange(1)
xrange = xmax-xmin
yrange = ymax-ymin
;
; find lines within x range and sort them
;
good = where((wline gt xmin) and (wline lt xmax),nlines)
if nlines lt 1 then return
wl = wline(good)
csize = csize(good) & cthick = cthick(good) & ethick = ethick(good)
txt1 = text1(good) & txt2 = text2(good)
sub = sort(wl)
wl = wl(sub) & csize = csize(sub) & ethick = ethick(sub)
chtick = cthick(sub)
txt1 = txt1(sub)
txt2 = txt2(sub)
es = string(format='(i5)',eqw)
txt2 = txt2+es(good)+' '+text3(sub)
maxids = 65/(total(csize)/nlines) ;maximum number of identifications
if nlines gt maxids then begin
print,'Too many lines to mark, print only first '+strtrim(fix(maxids),2)+' lines'
nlines=maxids
endif
;
; determine character height in wavelength units
;
char_height = abs(xrange) / 65 * csize
;
; adjust wavelengths of where to print the line ids
;
wlp = wl ;wavelength to print text
;
; test to see if we can just equally space the annotated lines
;
if (nlines gt maxids*0.85) and (n_elements(charsize) eq 1) then begin
wlp = findgen(nlines) * (xrange/(nlines-1)) + xmin
goto,print_text
end
;
; iterate to find room to annotate each line
;
changed = 1 ;flag saying we moved a wlp position
niter = 0
factor = 0.35 ;size of adjustments in text position
while changed do begin ;iterate
changed = 0
for i=0,nlines-1 do begin
;
; determine the difference of the annotation from the lines on the
; left and right of it and the required separation
;
if i gt 0 then begin
diff1 = wlp(i)-wlp(i-1)
separation1 = (char_height(i)+char_height(i-1))/2.0
end else begin
diff1 = wlp(i) - xmin + char_height(i)*1.01
separation1 = char_height(i)
end
if i lt (nlines-1) then begin
diff2 = wlp(i+1) - wlp(i)
separation2 = (char_height(i)+char_height(i+1))/2.0
end else begin
diff2 = xmax + char_height(i)*1.01 - wlp(i)
separation2 = char_height(i)
end
;
; determine if line annotation should be moved
;
if (diff1 lt separation1) or (diff2 lt separation2) then begin
if wlp(i) eq xmin then diff1 = 0
if wlp(i) eq xmax then diff2 = 0
if diff2 gt diff1 then $
wlp(i) = (wlp(i) + separation2*factor) < xmax $
else wlp(i) = (wlp(i) - separation1*factor) > xmin
changed = 1
endif
end
if niter eq 300 then $ ; fine adjustment for
factor = factor/3 ; crowded field
if niter eq 1000 then changed=0 ; stop at 1000 iterations
niter = niter + 1
endwhile
;
; print line id's
;
print_text:
maxcsize = max(csize)
start_arrow = ymax + yrange/60
bend1 = ymax + yrange/30
bend2 = ymax + (yrange/30)*3
stop_arrow = ymax + (yrange/30)*4
start_text1 = stop_arrow + yrange/50*maxcsize
start_text2 = start_text1 + $
max(strlen(strtrim(txt1,1)))*yrange/50*maxcsize
for i=0,nlines-1 do begin
plots,[wl(i),wl(i),wlp(i),wlp(i)], $
[start_arrow,bend1,bend2,stop_arrow]
xyouts,wlp(i) + char_height(i)/2, start_text1, txt1(i), $
orientation = 90, size=csize(i), charthick = cthick(i),_extra=pex
xyouts,wlp(i) + char_height(i)/2, start_text2, txt2(i), $
orientation = 90, size=csize(i), charthick = cthick(i),_extra=pex
endfor
;
; extend selected lines down to the spectrum
;
good = where((ethick gt 0) and (wl gt xmin) and (wl lt xmax),n)
if n lt 1 then return
ww = wl(good)
ethick = ethick(good)
; help,wave
; help,flux
; help,ww
; print,n_elements(wave)
; print,n_elements(flux)
; print,wline
linterp,wave,flux,ww,ff
ymax = !y.crange(1)
ymin = !y.crange(0)
offset = (ymax-ymin)/20.0
for i=0,n-1 do plots,[ww(i),ww(i)],[(ff(i)+offset)<ymax,ymax], $
line=2,thick = ethick(i),_extra=pex
return
end
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pro lineid_select,file,Wline,lineid,wstring,strength,eqw, $
ewlim=ewlim,n=n,range=range
;+
; lineid_select
;
; procedure to extract the wave and ID's from the SYNSPEC output file
; input: file=name of file
; output:Wline = real*8 vector of wavelengths
; lineid = vector of identifications (string array)
; wstring = string vector of wavelengths
; strength = string line strength indicator
; eqw = approximate equivalent width
; optional keyword inputs:
; ewlim = lower limit for approximate equivalent width
; (default = 0)
; N = strength indicator ( 0 1 2 3 4
; (' ','.' or '*' or '**' or '***')
; (default n = 2)
; range = 2 element vector giving desired wavelength range
; (default = [0,99999])
;-
;----------------------------------------------------------------------------
;
; print calling sequence
;
if n_params(0) lt 1 then begin
print,'CALLING SEQUENCE: lineid_select,file,Wline,lineid,'+ $
'wstring,strength,eqw'
print,'OPTIONAL KEYWORD PARAMETERS:'
print,' EWLIM = limiting approx. equivalent width'
print,' RANGE = [wmin,wmax] default=[0,99999]'
print,' N = minimum strength (0-5) default=2'
return
end
;
; set keyword defaults
;
if n_elements(N) eq 0 then N=2
if n_elements(ewlim) eq 0 then ewlim=0
if n_elements(range) eq 0 then range = [0,999999]
wmin = range(0)
wmax = range(1)
;
; open input file
;
close,1 & openr,1,file
;
; initialization for loop
;
st = ''
wline = dblarr(2000)
wstring = strarr(2000)
lineid = strarr(2000)
strength = strarr(2000)
eqw = fltarr(2000)
nlines = 0
;
; loop on lines in the file
;
while not eof(1) do begin
readf,1,st ;read string
st = strtrim(st,2) ;trim blanks
; for i=0,1 do junk=gettok(st,' ') ;skip first 2 columns. The old version of synspec required that
wave = gettok(st,' ') ;get wavelength
w = double(wave) ;convert to r*8
if (w ge wmin) and (w le wmax) then begin ;within range?
el = gettok(st,' ') ;element
; strput,el,strlowcase(strmid(el,1,1)),1 ;make second character
; lower case '
ion = gettok(st,' ')
for i=5,7 do junk = gettok(st,' ') ;skip columns 5-7
ew = double(gettok(st,' '))
str = strtrim(strmid(st,0,4),2) ;strength
case str of ;decode strength
'' : Nx=0
'.' : Nx=1
'*' : Nx=2
'**' : Nx=3
'***': Nx=4
else : Nx=999 ;unknown
endcase
;
; add line to the list
;
if Nx ge N and ew ge ewlim and nlines lt 2000 then begin
wline(nlines) = w
wstring(nlines) = wave + ' '
lineid(nlines) = el + ' ' + ion + ' '
strength(nlines) = str
eqw(nlines) = ew
nlines = nlines + 1
endif
end
end
;
; extract good part of the arrays
;
if nlines gt 0 then begin
wline = wline(0:nlines-1)
wstring = wstring(0:nlines-1)
lineid = lineid(0:nlines-1)
strength = strength(0:nlines-1)
eqw = eqw(0:nlines-1)
end else begin
print,'LINEID_SELECT: No lines found for given range/N'
end
close,1
return
end
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pro loadopt, file, optable,bin=bin
if n_params() lt 2 then begin
print,' LOADOPT,file,optable,/bin'
print,'file =STRING : name of the ASCII opacity table(input)'
print,'optable=STRUCT : loaded data from the optable (output)'
print,'/bin : the table is in binary format'
return
endif
defsysv,'!gdl',exist=gdl ; 1 is GDL , 0 is IDL
if keyword_set(bin) then begin
openr, lun, file, /f77_un,/get_lun
type = STRARR(30)
abnd = FLTARR(30)
abnd2 = FLTARR(30)
hdr='opacity table with element abundances:'
hdr=[hdr,'element for EOS for opacities']
FOR ii = 0, 29 DO begin
a = 'aaaa'
b = 0.D
c = 0.D
READU,lun, a, b, c
; PRINT, a, b, c
type[ii]=a & abnd[ii]=b & abnd2[ii]=c
hdr=[hdr,string(a,b,c,format='(3x,a4,2e12.3E3)')]
ENDFOR
hdr=[hdr,'']
hdr=[hdr,'molecules - ifmol,tmolim:']
ifmol = LONG(0)
tmolim = 0.D0
READU,lun, ifmol, tmolim
; print, ifmol, tmolim
hdr=[hdr,string(ifmol,tmolim,format='(3x,i4,f12.1)')]
hdr=[hdr,'additional opacities']
hdr=[hdr,' H- H2+ He- CH OH']
iophmp = LONG(0)
ioph2p = LONG(0)
iophem = LONG(0)
iopch = LONG(0)
iopoh = LONG(0)
READU,lun, iophmp,ioph2p,iophem,iopch,iopoh
; print, iophmp,ioph2p,iophem,iopch,iopoh
hdr=[hdr,string(iophmp,ioph2p,iophem,iopch,iopoh,format='(5i4)')]
hdr=[hdr,'']
hdr=[hdr,'number of frequencies, temperatures, densities:']
nfgrid = LONG(0)
ntemp = LONG(0)
ndens = LONG(0)
READU,lun, nfgrid,ntemp,ndens
; PRINT, nfgrid,ntemp,ndens
temp = DBLARR(ntemp)
dens = DBLARR(ndens)
elec = DBLARR(ntemp, ndens)
READU,lun, temp
READU,lun, dens
READU,lun, elec
; absgrd = DBLARR(ntemp, ndens, nfgrid)
opt=DBLARR(nfgrid,ntemp,ndens)
wlgrid = DBLARR(nfgrid)
FOR k = 0L, nfgrid-1 DO BEGIN
w = 0.D0
READU,lun, w
wlgrid[k] = w
FOR j = 0, ndens-1 DO BEGIN
abs = FLTARR(ntemp)
READU,lun, abs
; absgrd[*, j, k] = abs
opt[k,*, j] = abs
; print, abs
ENDFOR
ENDFOR
close,lun & free_lun,lun
optable={hdr:hdr,wave:wlgrid,temp:exp(temp),rho:exp(dens),nel:exp(transpose(elec)),opt:opt}
return
endif
openr,lun,file,/get_lun
line=''
; read header ...
readf,lun,line ; 'opacity table with element abundances:'
hdr=line
readf,lun,line ; 'element for EOS for opacities'
while strpos(line,'frequenc') eq -1 and strpos(line,'temper') eq -1 do begin
hdr=[hdr,line]
readf,lun,line
endwhile
readf, lun, line ; numfreq numtemp numrho
kas=strsplit(line,' ',/extract)
numfreq=long(kas[0])
numtemp=long(kas[1])
numrho=long(kas[2])
opt=dblarr(numfreq,numtemp,numrho)
topt=dblarr(numtemp,numrho)
lambda=dblarr(numfreq)
readf,lun,line ; "log temperatures"
if strtrim(line,2) ne 'log temperatures' then stop,'Temperatures not where they should be. Check op table '
readf,lun,line ; array of temperatures
tempvec=strsplit(line,' ',/extract)
if n_elements(tempvec) ne numtemp then begin
repeat begin
readf,lun,line
tempvec=[tempvec,strsplit(line,' ',/extract)]
endrep until n_elements(tempvec) eq numtemp
endif
readf,lun,line ; "log densities"
if strtrim(line,2) ne 'log densities' then stop,' Densities not where they should be. Check op table '
readf,lun,line ; array of temperatures
rhovec=strsplit(line,' ',/extract)
if n_elements(rhovec) ne numrho then begin
repeat begin
readf,lun,line
rhovec=[rhovec,strsplit(line,' ',/extract)]
endrep until n_elements(rhovec) eq numrho
endif
readf,lun,line ; "log electron densities from EOS"
nel=dblarr(numtemp,numrho)
nel=transpose(nel)
ii=0
repeat begin
readf,lun,line
kas=strsplit(line,' ',/extract)
nel[ii : ii+n_elements(kas)-1]=double(kas)
ii+=n_elements(kas)
endrep until ii eq numtemp*numrho
nel=transpose(nel) ; to have it nel[ntemp,ndens]
line=findline(lun,'frequency') ; '*** frequency # :' ind lambda
kas=strsplit(line,' ',/extract)
lambda[0]=double(kas[-1])
readf,lun,line ; frequency
freqvec=double(line)
readf,lun,line
kas=double(strsplit(line,' ',/extract))
repeat begin
readf,lun,line
kas=[kas,double(strsplit(line,' ',/extract))]
endrep until n_elements(kas) eq numtemp*numrho
topt[*]=kas
opt[0,*,*]=topt
for ii=2L, numfreq do begin
; for ii=2, 1000 do begin
readf,lun,line ; empty line
readf,lun,line ; '*** frequency # :' ind lambda
kas=strsplit(line,' ',/extract)
lambda[ii-1]=double(kas[-1])
if ii mod 100 eq 0 then progress,'',round((ii*100)/(numfreq)),' % '
readf,lun,line ; frequency
freqvec=[freqvec,double(line)]
readf,lun,line
kas=double(strsplit(line,' ',/extract))
; kas[where(kas eq 0.)]=-99.00
repeat begin
readf,lun,line
kas=[kas,double(strsplit(line,' ',/extract))]
if n_elements(kas) gt numtemp*numrho then stop,'something is wrong in the opacity table !'
endrep until n_elements(kas) eq numtemp*numrho
topt[*]=kas
opt[ii-1,*,*]=topt
endfor
print,''
close,lun
free_lun,lun
optable={hdr:hdr,wave:lambda,temp:exp(tempvec),rho:exp(rhovec),nel:exp(nel),opt:opt}
end
pro printopt,opt,fileout
if n_params() eq 0 then begin
print,' prints the opacity table.'
print,' printopt,opt,fileout'
print,''
return
endif
openw,lun,fileout,/get_lun
for ii=0,n_elements(opt.hdr)-1 do printf,lun,opt.hdr[ii]
clight=2.99792548d18
printf,lun,'number of frequencies, temperatures, densities: '
nfr=n_elements(opt.wave)
nt=n_elements(opt.temp)
nr=n_elements(opt.rho)
printf,lun,nfr,nt,nr,format='(10x,3i10)'
printf,lun,'log temperatures'
printf,lun,alog(opt.temp),format='(6f11.6)'
printf,lun,'log densities'
printf,lun,alog(opt.rho),format='(6f11.6)'
printf,lun,'log electron densities from EOS'
printf,lun,alog(transpose(opt.nel)),format='(6f11.6)'
for ii=0L, nfr-1 do begin
printf,lun,''
printf,lun,ii+1,opt.wave[ii],format='(" *** frequency # :",i9,f15.5)'
printf,lun,clight/opt.wave[ii],format='(e20.8E3)'
for jj=0, nr-1 do printf,lun,opt.opt[ii,*,jj],format='(6E14.6E3)'
endfor
close,lun
free_lun,lun
end
+111
View File
@@ -0,0 +1,111 @@
pro plotspec,ident,name,rv=rv,xrange=xr,lxrange=lxr,list_elem=elist,relative=relative,elem=ielem,_extra=pex,fwhm=fwhm,viewp=viewp,idsize=idsize
;
; made by Yeisson Osorio Feb 2020
;
if n_params() lt 2 then begin
print,"plotspec,ident,name,rv=rv,fwhm=fwhm,xrange=xr,elem=elem,idsize=idsize,_extra=pex"
print," ident = (real) if 0 just plot, if > 0 plot names of lines with weq >= iden (mAngs)"
print," name = (str) name of synspec output files (with no sufix)"
print," lxr = (real[2]) wavelength range to consider (default whole range)"
print," rv = (real) radial velocity shift"
print," elem = (str[]) name of the element(s) to plot (if empty plot all)"
print," list_elem = (output) list of visible elements"
return
endif
defsysv,'!gdl',exist=gdl ; 1 is GDL , 0 is IDL
if keyword_set(ielem) then elem=strtrim(ielem,2)+' '
if n_elements(xr) eq 0 then xr=[0,0]
if ident gt 0 and ~gdl then begin
if n_elements(viewp) eq 4 then vp=viewp else vp=[0.13,0.95,0.1,0.65]
set_viewport,vp[0],vp[1],vp[2],vp[3]
endif
if ident gt 0 and gdl then !p.position=[0.075,0.1,0.95,0.65]
if name eq 'fort' then begin
if keyword_set(relative) then rotin,'fort.7','fort.17','fort.10',/relative,wl,fl else readcol,'fort.7',wl,fl,format='(d,d)'
endif else begin
if keyword_set(relative) then readcol,name+'.10',wl,fl,format='(d,d)',/silent else readcol,name+'.7',wl,fl,format='(d,d)',/silent
endelse
wstart= xr[0] eq 0 ? min(wl) : xr[0]
wend = xr[1] eq 0 ? max(wl) : xr[1]
wl=reform(wl)
fl=reform(fl)
if n_elements(fwhm) eq 1 or n_elements(rv) eq 1 then fl=fconvol(wl,fl,wl,fwhm=fwhm,rv=rv)
plot,wl,fl,xr=xr,_extra=pex
if ident gt 0 then begin
if n_elements(extend) gt 0 then begin
if iplot ge 0 then begin
nln=n_elements(wl)
wla=fltarr(nln)
fla=wla
for i=0,nln-1 do begin wla(i)=wl(i) & fla(i)=fl(i) & endfor
endif
if n_elements(observ) eq 1 then begin
nobs=n_elements(wlobs)-1
if iplot ge 0 then beyond=wl(nln-1) lt wlobs(0) or wl(0) gt wlobs(nobs-1)
if iplot lt 0 then beyond=1
if extend lt 0 then begin
extend = -extend
beyond=1
endif
nln=n_elements(wlobs)
wla=fltarr(nln)
fla=wla
for i=0,nln-1 do begin wla(i)=wlobs(i) & fla(i)=flobs(i) & endfor
endif
endif
if keyword_set(lxr) then ra=lxr else ra=[wstart,wend]
ewl=ident
; the new version of synspec has fort.14 formatted the
; following way:
; 2 1 3721.935 H I -1.97 82259.250 1.06E-02 0.9 . 2 14
; and should be
; 3721.935 H I -1.97 82259.250 1.06E-02 0.9 . 2 14
;
if name eq 'fort' then begin
if file_test('fort.15') then begin
spawn,"sed 's/^\(.............\)\(....\) /\1 \2 ./g' fort.15 > f15"
spawn,'cat fort.12 f15 | sort -n -k 3,3 >| f12'
endif else spawn,"cp fort.12 f12"
endif else begin
if file_test(name+'.15') then begin
spawn,"sed 's/^\(.............\)\(....\) /\1 \2 ./g' "+name+".15 > f15"
spawn,'cat '+name+'.iden f15 | sort -n -k 3,3 >| f12'
endif else spawn,"cp "+name+".12 f12"
endelse
spawn,'rm tf12'
if n_elements(elem) ne 0 then begin
for ii=0, n_elements(elem)-1 do begin
kas=strsplit(elem[ii],' ',/extract)
if n_elements(kas) eq 1 then spawn,'grep "'+kas+'" f12 >> tf12' $
else spawn,'grep "'+kas[0]+'" f12 | grep "'+kas[1]+'" >> tf12'
endfor
spawn,'sort -n -k 3,3 tf12 > f12'
endif else begin
spc='" "'
spawn,"awk '{print $2"+spc+"$3}' f12 | sort -u > tf12"
readcol,'tf12',a,i,format='(a,a)',/silent
elist=a+' '+i
elist=strtrim(repstr(elist,'.',''),2)
endelse
line="awk '{if ($1 >= "+strtrim(min(ra),2)+" && $1 <= "+strtrim(max(ra),2)+") print $0 }' f12 > tf12"
spawn,line
if ident lt 1 then N=0 else N=2
lineid_select,'tf12',wli,lid,wst,st,ew,ewlim=ewl,range=ra,N=N
if n_elements(rv) eq 1 then $
wli=wli*(1.-rv/2.9977925e5)
if keyword_set(pex) then begin
dum=where(strpos(tag_names(pex),'CO') ne -1)
if dum ne -1 then dum=pex.(dum) else dum=!p.color
endif
lineid_annot,wla,fla,wli,ew,lid,wst,charsize=idsize,extend=extend,col=dum
if ~gdl then set_viewport
endif
end
+961
View File
@@ -0,0 +1,961 @@
pro synplot,ispec,iplot,ident,wl,fl,eqw,sp,wlobs=wlobs,flobs=flobs, $
atmos=atmos,linlist=linlist,input=input,abund=abund, $
imode=imode,idstd=idstd,iprin=iprin, $
kurucz=kurucz,oldinp=oldinp,disk=disk, $
cont=cont,nlte=nlte,lyman=lyman,vturb=vturb, $
optab=optab,optemp=optemp,opdens=opdens,nlamb=nlamb, $
bintab=bintab,relabn=relabn,inttab=inttab, $
wstart=wstart,wend=wend,wdist=wdist, $
cutoff=cutoff,strength=strength,icontl=icontl,ifhe2=ifhe2, $
hydprf=hydprf,he1prf=he1prf,he2prf=he2prf, $
nangles=nangles,anglmin=anglmin, $
vrot=vrot,vmac=vmac,steprot=steprot,fwhm=fwhm,stepins=stepins, $
relative=relative,scale=scale,rv=rv, $
extend=extend,charsize=charsize,lidshift=lidshift, $
observ=observ,noread=noread,spect=spect,inlist=inlist, $
save=save,f55=f55,molecules=molecules,ichang=ichang,_extra=e
;
;
; program for ploting spectra calculated by SYNSPEC,
; with a possibility to change interactively the chemical composition;
; and interactively convolved with rotation and instrumental broadening;
; and possibly also annotated by line identifications
;
; written by I. Hubeny, Nov-Dec 1994
; modified - Jul 1996
; further modified - Nov 1996
; May 1997
; modified - Yeisson Osorio Jul 2018
; - added optab and relabn for constructing opacity tables
; - added f55 option to use another fort.55 file (use with
; caution! )
;
; ispec = 0 - Synspec is run
; no change of chemical composition;
; < 0 - Synspec is not run (only Rotins is run)
; > 0 - ispec elements change abundance; entered interactively
; iplot = 0 - original plot
; = 1 - overplot, IPLOT has the meaning of the color index
; ident = 0 - identification is not plotted
;
; OPTIONAL KEYWORD INPUT:
;
; ATMOS - file name(s) for a model atmosphere
; LINLIST - filename of the line list
; INPUT - filenames of the additional input (usually not set)
; OBSERV - filename of the observed spectrum
; IMODE - basic mode of SYNSPEC
; KURUCZ - switch for indicating a Kurucz model input (if =1)
; NLTE - NLTE switch (see SYNSPEC)
; LYMAN - switch for treating Lyman lines (IOPHLI in Synspec)
; VTURB - turbulent velocity (in km/s)
;
; OPTAB - name of output file with the opacity table
; optemp - optemp = [NTEMP, TEMP1, TEMP2]
; opdens - opdens = [IDENS, NDENS, DENS1, DENS2] not defined
; nlamb - number of wavelength points
; inttab - transformation mode from internal to universal
; wavelength points
; /bintab - output table in binary mode (default ascii)
; RELABN - pairs (IATOM, RELABN) for op tables
;
; WSTART - starting wavelength (in Angstrom)
; WEND - final wavelength (in A)
; WDIST - step in wavelength
; STRENGTH - criterion for selecting lines (RELOP in Synspec)
; CUTOFF - distance in A to which lines are allow to contribute
; IFHE2 - He II opacity switch (see SYNSPEC)
;
; VROT - rotational velocity - v sin i (in km/s)
; VMAC - macro-turbulent velocity - (in km/s)
; STEPROT - step for the rotational convolution (if non-zero)
; FWHM - FWHM for the instrumental profile (in A)
; STEPINS - step for instrumental convolution (if non-zero)
; RELATIVE - switch for computing relative spectrum (if =1)
; SCALE - a scale factor to multiply the theoretical spectrum
; RV - radial velocity (in km/s) applied on theor. spectrum
;
; EXTEND - switch for drawing vertical lines in identification
; CHARSIZE - character size in identification
;
; ABUND - vector of abundance changes
; SAVE - core filename for saved files
;
; _EXTRA - a set of any extra keywords for PLOT
;
if n_params(0) eq 0 then begin
print,'pro synplot,ispec,iplot,ident,eqw,sp,flobs,wlobs, '
print,'OPTIONAL KEYWORD PARAMETERS '
print,' type 1 for a short list;'
print,' 2 for a long list with explanations;'
print,' else return'
read,ii
if ii eq 1 then begin
print,'atmos,linlist,input,observ, (filenames)'
print,'imode,idstd,kurucz,nlte,lyman,vturb (fort.55 for SYNSPEC)'
print,'wstart,wend,wdist,strength,cutoff,ifhe2,icontl, (still fort.55)'
print,'hydprf,he1prf,he2prf, (H, HeI, HeII line broadening tables-fort.55)'
print,'nangles,anglmin (still fort.55)'
print,'vrot,vmac,steprot,fwhm,stepins,relative, (for ROTINS)'
print,'scale,rv, (radial velocity and scaling of the final spectrum)'
print,'optab,optemp,opdens,inttab,nlamb,bintab,relabn, (for opacity tables )'
print,'extend,charsize, (for LINEID)'
print,'abund,noread,spect,save,_extra (miscellaneous)'
endif else begin
if ii eq 2 then begin
print,'POSITIONAL PARAMETERS:'
print,''
print,'ispec = 0 - normal run of Synspec; <0 - (no run of Synspec),'
print,' >0 - ispec abundances changed'
print,'iplot = 0 - first plot; >0 oplot (iplot is the color index)'
print,' <0 - plot only the observed spectrum'
print,'ident = 0 - no identification; >0 - identification'
print,' in that case, lines with eqw > ident mA are marked'
print,'eqw - output: total equivalent width (in mA)'
print,'sp - if present, an array of synthetic spectrum (generated'
print,' by a previous run of Synplot)'
print,'wlobs - if present, array of wavelengths of the observed spectrum'
print,'flobs - if present, array of fluxes of the observed spectrum'
print,''
print,'KEYWORD PARAMETERS:'
print,'atmos - names(s) for the input model atmosphere (disk)'
print,' if absent: either not needed, or assumed to be'
print,' fort.5 (std input) and fort.8 (model)'
print,' if a single string: generic name'
print,' files are atmos.5 and atmos.7'
print,' if a 2-comp string vector: '
print,' files are atmos(0) and atmos(1)'
print,'oldinp - if set, the "old" format of input (up to tlus194,syn41)'
print,'disk - if set, input accretion disk model is assumed'
print,'linlist - filename for the line list (default fort.19)'
print,'input - names(s) for the additional input to Synspec'
print,' (unit 55) and Rotins (std input)'
print,' default - SYNPLOT creates these files'
print,' if present, it must be a 2-comp string vector,'
print,' [filename for unit55, std input to Rotins]'
print,'abund - if present, it is another method to change abundances'
print,' must be vector [first at.number, last a.num., abund],'
print,' or more triads consecutively'
print,''
print,'imode - basic mode of Synspec (default 0)'
print,'cont - the same as imode=2 - flux in continuum'
print,'idstd - standard depth; if not set, the program assigns'
print,' the last depth point where T<Teff'
print,'kurucz - if =1, Kurucz model atmosphere, otherwise Tlusty'
print,' (default 0 - Tlusty)'
print,'nlte - NLTE switch in Synspec'
print,' (default 1 - NLTE lines, if NLTE populations given)'
print,'lyman - switch for the treatment of Lyman lines (default 1)'
print,'vturb - turbulent velocity (in km/s) - default 0'
print,''
print,'wstart - starting wavelength (in A)'
print,'wend - end of the wavelength interval (in A)'
print,'wdist - (maximum) wavelength step (in A) - default 0.01'
print,'strength - criterion for rejecting lines - default 1.e-4'
print,'icontl - switch for considering H lines as continua'
print,'ifhe2 - switch for treatment He II lines - default 0'
print,'hydprf - filename for the special H line broadening table'
print,'he1prf - filename for the special HeI line broadening table'
print,'he2prf - filename for the special HeII line broadening table'
print,'nangles- if set, the number of angles for evaluating intensity'
print,' equidistant mu''s between 1 and anglmin'
print,'anglmin- minimum mu = cos(angle) for evaluating intensity'
print,' default = 0.1'
print,''
print,'vrot - rotational velocity (in km/s) - default 0'
print,' < 0 - ROTIN is not called'
print,'vmac - macroturbulent velocity (in km/s) - default 0'
print,'steprot - wavelength step for rotated spectra (in A),'
print,' default = (wstart+wend)*vrot/c/5'
print,'fwhm - FWHM for (Gaussian) instrumental profile (default 0)'
print,' < 0 - ROTIN is not called'
print,'stepins- step for convolved spectra (default fwhm/10)'
print,'relative - if nonzero, plot relative spectrum (default 0)'
print,'scale - scale factor for synthetic spectra (default 1)'
print,'rv - radial velocity (in km/s) to be applied '
print,' to synthethic spectra (default 0)'
print,''
print,'optab - name of the file with the opacity table'
print,'optemp - [NTEMP, TEMP1, TEMP2]'
print,'opdens - [IDENS, NDENS, DENS1, DENS2]'
print,'nlamb - number of waelenght points for the opacity table'
print,'inttab - transformation mode from internal to universal'
print,' wavelength points (1 interpolation of wavelenghts '
print,' default = 0 by integral over wavelengths )'
print,'bintab - if 1 optable is in binary mode, default 0 (= ascii)'
print,'relabn - changes in chemical abundances in the opa table'
print,' is an arrya of pairs:'
print,' [[z1,rel1],[z2,rel2],...]'
print,' where zi is atomic number and reli multiplication'
print,' factor of the input abundance (typically 0)'
print,''
print,'extend - swich for drawing lines for identification'
print,'charsize - character size in identification (default 1)'
print,'lidshift - if set, identification is shifted with rv'
print,''
print,'observ - if present, and is a string, then it is the'
print,' the filename of the observed spectrum;'
print,' (simple table wavelength (in A) vers. flux(any units))'
print,' - if present, and is equal to number 1, '
print,' then it indicates that the observed spectrum is'
print,' on positional parameters WLOBS and FLOBS'
print,'noread - if present and non-zero, the synthetic spectrum is'
print,' not read from the file fort.10 (must be transfered'
print,' by positional parameter SP)'
print,'spect - has an effect only if NOREAD is not set,'
print,' and if the spectrum is not computed by the present run:'
print,' the filaneme where the synthetic spectrum is stored'
print,' (if it is different from fort.10)'
print,''
print,'save - if present, filename for saving created files'
print,' with filenames save+.7, save+.17, etc'
print,'_extra - any extra keywords for IDL routine PLOT'
endif else return
endelse
return
endif
; check op system
spawn,'uname',opsys
opsys=strlowcase(strtrim(opsys,2))
case opsys of
'linux' : begin
synspec='synspec.linux'
rotin='rotin.linux'
end
'darwin': begin
synspec='synspec.mac'
rotin='rotin.mac'
end
else: begin
message,'# WARNING: I am not sure the OS you are running me on... ',/cont
synspec='synspec.exe'
end
endcase
;
; initialization
;
if n_elements(atmos) eq 1 then begin
fort5=atmos+".5"
fort8=atmos+".7"
endif
if n_elements(atmos) eq 2 then begin
fort5=atmos(0)
if fort5 eq 'cool.5' then oldinp=1
fort8=atmos(1)
endif
;
if n_elements(inlist) eq 0 then inlist=10
if n_elements(ichang) eq 0 then ichang=0
if n_elements(linlist) eq 1 then begin
if linlist ne 'fort.19' then begin
a='ln -s -f '+linlist+' fort.19'
spawn,a
endif
endif
;
if n_elements(abund) ne 0 then ichemc=1 else ichemc=0
if n_elements(imode) eq 0 then imode=0
if keyword_set(cont) then imode=2
if keyword_set(optab) then iopt=1 else iopt=0
if n_elements(kurucz) eq 0 then inmod=1 else begin
if kurucz ge 0 then inmod=0 & endelse
if ispec ge 0 then begin
if strmid(fort8,0,5) eq 'ap00t' then inmod=0
endif
if keyword_set(disk) then inmod=2
if keyword_set(nlte) then nlte=1 else nlte=0
;if inmod eq 0 then nlte=0
if n_elements(icontl) eq 0 then icontl=0
if n_elements(ifhe2) eq 0 then ifhe2=0
if n_elements(lyman) eq 0 then lyman=0
;
; set up parameteres for special line broadening tables
;
if n_elements(hydprf) eq 0 then ihydpr=0 else ihydpr=hydprf
;else begin $
; ihydpr=20
; spawn,'rm -f fort.20'
; hydprf=strtrim(string(hydprf),2)
; if hydprf ne '1' then begin
; a='ln -s '+hydprf+' fort.20'
; spawn,a
; endif else begin
; spawn,'ln -s hydprf.dat fort.20'
; hydprf='hydprf.dat'
; endelse
;endelse
if n_elements(he1prf) eq 0 then ihe1pr=0 else begin $
ihe1pr=21
spawn,'rm -f fort.21'
he1prf=strtrim(string(he1prf),2)
if he1prf ne '1' then begin
a='ln -s '+he1prf+' fort.21'
spawn,a
endif else begin
spawn,'ln -s he1prf.dat fort.21'
he1prf='he1prf.dat'
endelse
endelse
if n_elements(he2prf) eq 0 then ihe2pr=0 else begin $
ihe2pr=22
spawn,'rm -f fort.22'
he2prf=strtrim(string(he2prf),2)
if he2prf ne '1' then begin
a='ln -s '+he2prf+' fort.22'
spawn,a
endif else begin
spawn,'ln -s he2prf.dat fort.22'
he2prf='he2prf.dat'
endelse
endelse
if n_elements(cutoff) eq 0 then if iopt then cutoff=50.0 else cutoff=100.00
if n_elements(strength) eq 0 then if iopt then strength=1.e-3 else strength =1.e-4
if n_elements(wdist) eq 0 then begin
if imode ne 2 then begin
if iopt then wdist=0.12 else wdist=0.01
endif else wdist=0.5
endif
;
close,1 ; in case unit 1 is open!
;
if ispec ge 0 then begin
if n_elements(wstart) eq 0 then begin
spawn,'head -1 fort.19 >| lin1.tmp'
openr,1,'lin1.tmp'
readf,1,al1
close,1
wstart=al1*10.
if imode eq 1 then wstart=wstart-cutoff*0.5
endif
;
if n_elements(wend) eq 0 then begin
spawn,'tail -1 fort.19 >| lin2.tmp'
openr,1,'lin2.tmp'
readf,1,al2
close,1
wend=al2*10.
if imode eq 1 then wend=wend+cutoff*0.5
endif
endif else begin
nmlist=fix(n_elements(molecules))
if n_elements(wstart) eq 0 then begin
spawn,'head -1 fort.7 >| lin1.tmp'
openr,1,'lin1.tmp'
readf,1,al1
close,1
wstart=al1
endif
;
if n_elements(wend) eq 0 then begin
spawn,'tail -1 fort.7 >| lin2.tmp'
openr,1,'lin2.tmp'
readf,1,al2
close,1
wend=al2
endif
endelse
;
if n_elements(vrot) eq 0 then vrot=0.
if n_elements(steprot) eq 0 then steprot=0
if n_elements(fwhm) eq 0 then fwhm=0.
if n_elements(stepins) eq 0 then stepins=0
if n_elements(relative) eq 0 then relative=0
if n_elements(scale) eq 0 then scale=1.
if n_elements(rv) eq 0 then rv=0.
if n_elements(iprin) eq 0 then iprin=0
;
;
if ispec ge 0 then begin
;
; construct the input file fort.55 for Synspec
;
if n_elements(input) eq 0 then begin
if iopt then begin
idstd=1
imode-=3
endif
if n_elements(idstd) gt 0 then idst=idstd else begin
idst=0
; if inmod eq 0 or inmod eq 2 then idst=0 else begin
; a='grep -v "*" '+fort5+' |head -1 >| tetmp'
; spawn,a
; close,1 & openr,1,'tetmp'
; readf,1,teff,grav
; close,1 & openr,1,fort8
; readf,1,nd,np
; np=abs(np) ; check consequenses !!
; dm=fltarr(nd)
; readf,1,dm
; parm=fltarr(np,nd)
; readf,1,parm
; temp=parm(0,*)
; for id=0,nd-1 do if temp(id) lt teff then ids=id
; idst=ids+1
; endelse
endelse
close,1
if keyword_set(molecules) then begin
nmlist=fix(n_elements(molecules)) & mols=fix(molecules)
endif else begin
nmlist=0 & mols=0
endelse
if ~keyword_set(f55) then begin
openw,1,'f55'
zero=0
one=1
printf,1,imode,idst,iprin
printf,1,inmod,zero,ichang,ichemc
printf,1,lyman,zero,zero,zero,zero
printf,1,one,nlte,icontl,inlist,ifhe2
printf,1,ihydpr,ihe1pr,ihe2pr
if iopt then printf,1,wstart,-abs(wend),cutoff,2000,strength,wdist $
else printf,1,wstart,wend,cutoff,zero,strength,wdist
printf,1,nmlist,mols
noturb=0
if n_elements(vturb) eq 1 then printf,1,vturb else noturb=1
if keyword_set(nangles) then begin
if n_elements(anglmin) eq 0 then anglmin=0.1
if noturb eq 1 then printf,1,-1
iflux=1
printf,1,nangles,anglmin,iflux
if nangles lt 0 then begin
print,'enter ',-nangles,' values of mu=cos(angle)'
ang=fltarr(-nangles)
read,ang
printf,1,ang
endif
endif
close,1
spawn,'/bin/cp f55 fort.55'
endif else spawn,'/bin/cp '+f55+' fort.55'
endif
;
; construct the input file fort.2 (rel abn for op tables) for Synspec
;
if iopt then begin
if n_elements(inttab) eq 0 then inttab=0
if n_elements(optemp) ne 3 then begin
print,'optemp = [NTEMP, TEMP1, TEMP2] not defined'
return
endif
if n_elements(opdens) ne 4 then begin
print,'opdens = [IDENS, NDENS, DENS1, DENS2] not defined'
return
endif
if n_elements(nlamb) ne 1 then begin
print,'nlamb = NLAMB not defined'
return
endif
openw,1,'fort.2'
printf,1,optemp,format='(i-5,2e-15.3e3)'
printf,1,opdens[0],format='(i-5)'
printf,1,opdens[1:*],format='(i-5,2e-15.3e3)'
printf,1,nlamb,inttab,wstart,wend,format='(i-12,i-3,2f15.0)'
printf,1,"'"+strtrim(optab,2)+"'",fix(keyword_set(bintab))
;
; construct the input file fort.3 (rel abn for op tables) for Synspec
;
if keyword_set(relabn) and iopt then begin
dum=size(relabn)
if dum[1] ne 2 then begin
print,'relative abundance for opacity table not used (wrong array`s format)'
endif else begin
for i=0, n_elements(relabn[0,*])-1 do begin
printf,1,relabn[*,i],format='(i4,f15.4)'
endfor
endelse
endif
close,1
if iopt then begin
print,'opacity table constructed with'
print,'FORT.2 : '
print,'--------------'
spawn,'cat fort.2'
print,'--------------'
print,''
endif
endif
;
; construct the input file fort.56 for Synspec
;
openw,1,'inp.tmp'
if ispec le 0 then begin
izer=0
if n_elements(abund) eq 0 then printf,1,izer
endif else begin
;
; interactive input of abundances
;
for i=1,ispec do begin
print,'enter starting and ending atomic number, abund'
read,ia0,ia1,abun
for ia=ia0,ia1 do printf,1,ia,abun,format='(i10,f10.3)'
endfor
endelse
;
; input of abundances as a parameter ABUND
;
if n_elements(abund) ge 3 then begin
ichemc=1
ispec=n_elements(abund)/3
for i=0,ispec-1 do begin
for ia=abund(3*i),abund(3*i+1) do printf,1,ia,abund(3*i+2),$
format='(i4,e15.4)'
endfor
endif else ichemc=0
close,1
if n_elements(abund) gt 0 or ispec gt 0 then begin
spawn,'wc -l inp.tmp > inum.tmp'
spawn,'sed s/inp.tmp// inum.tmp > inum1.tmp'
spawn,'cat inum1.tmp inp.tmp > fort.56'
endif else begin
spawn,'/bin/cp inp.tmp fort.56'
endelse
;
; construct the input file fort.1 for Synspec
;
i=0
if keyword_set(oldinp) then i=1
openw,1,'f1'
printf,1,i
close,1
spawn,'/bin/cp -f f1 fort.1'
;
if n_elements(optab) eq 0 then begin
a='/bin/cp '+fort8+' fort.8'
spawn,a
endif
;
a='./'+synspec+' < '+fort5+' > sylog.tmp'
;
spawn,a
if n_elements(optab) eq 0 then begin
spawn,'tail -1 fort.16 > eq.tmp'
openr,1,'eq.tmp'
readf,1,t1,t2,t3,t4,eqw1
print,'total equivalent width: ',eqw1,' milliangstrom'
close,1
eqw=eqw1
endif else begin
save=strsplit(optab,'.',/extract)
if n_elements(save) gt 1 then begin
save=save[0:n_elements(save)-2]
save=strjoin(save,'.')
endif
a='/bin/mv sylog.tmp '+save+".log"
spawn,a
return
endelse
endif
;
; -------------------------------------------------------------------------------
;
if ident gt 0 then set_viewport,0.13,0.95,0.1,0.65
if ~keyword_set(vmac) then vmac=0.0
if vrot ge 0 and fwhm ge 0 then begin
;
; construct the input file for rotins
;
openw,1,'r.tmp'
printf,1," 'fort.7' 'fort.17' 'fort.10' "
printf,1,vrot,wdist,steprot
printf,1,fwhm,stepins,vmac
printf,1,wstart,wend,relative
close,1
;
; run rotins
;
spawn,'./'+rotin+' <r.tmp > out.tmp'
endif else spawn,'/bin/cp -f fort.7 fort.10'
;
; -------------------------------------------------------------------------------
;
if n_elements(noread) eq 0 then begin
if n_elements(spect) ne 0 then begin
a='/bin/cp -f '+spect+' fort.10'
spawn,a
endif
spawn,'wc -l fort.10 >| eq.tmp'
openr,1,'eq.tmp'
readf,1,npt
close,1
openr,1,'fort.10'
sp=fltarr(2,npt)
readf,1,sp
close,1
endif
;
; -------------------------------------------------------------------------------
;
ymax=1
if relative gt 0 and iplot eq 0 then begin
ym=max(sp(1,*))
if ym le 1 and ym ge 0.8 then ymax=1.2
if ym gt 1.2 then ymax=ym
set_xy,0,0,0,ymax
endif
;
; apply scale factor (scale) and radial velocity (rv) to the convolved spectrum
; (if required)
;
if n_elements(scale) eq 0 then fl=reform(sp(1,*)) else fl=reform(sp(1,*))*scale
if n_elements(rv) eq 0 then wl=reform(sp(0,*)) else wl=reform(sp(0,*))*(1.+rv[0]/2.9977925e5)
if iplot le 0 then begin
;
; read and plot the observed spectrum (if required)
;
if n_elements(observ) eq 0 then plot,wl,fl,_extra=e else begin
observ=strtrim(string(observ),2)
if observ ne '1' then begin
close,1 & openr,1,observ
i=0L
wlobs=fltarr(35000) & flobs=wlobs
while not eof(1) do begin
readf,1,wl0,fl0
wlobs(i)=wl0
flobs(i)=fl0
i=i+1L
endwhile
nobs=i-1L
wlobs=wlobs(0:nobs)
flobs=flobs(0:nobs)
endif
plot,wlobs,flobs,xr=[wstart,wend],ps=sym(1),symsize=0.5,_extra=e
if iplot eq 0 then oplot,wl,fl
endelse
endif else begin
; if iplot le 256 then oplot,wl,fl,color=iplot_extra=e else oplot,wl,fl,_extra=e
oplot,wl,fl,_extra=e
endelse
set_xy
close,1
;
;
; if required (ident > 0), do graphical identification
;
if ident gt 0 then begin
if n_elements(extend) gt 0 then begin
if iplot ge 0 then begin
nln=n_elements(wl)
wla=fltarr(nln)
fla=wla
for i=0,nln-1 do begin wla(i)=wl(i) & fla(i)=fl(i) & endfor
endif
if n_elements(observ) eq 1 then begin
nobs=n_elements(wlobs)-1
if iplot ge 0 then beyond=wl(nln-1) lt wlobs(0) or wl(0) gt wlobs(nobs-1)
if iplot lt 0 then beyond=1
if extend lt 0 then begin
extend = -extend
beyond=1
endif
nln=n_elements(wlobs)
wla=fltarr(nln)
fla=wla
for i=0,nln-1 do begin wla(i)=wlobs(i) & fla(i)=flobs(i) & endfor
endif
endif
ra=[wstart,wend]
ewl=ident
; the new version of synspec has fort.14 with formated
; the following way:
; 2 1 3721.935 H I -1.97 82259.250 1.06E-02 0.9 . 2 14
; and should be
; 3721.935 H I -1.97 82259.250 1.06E-02 0.9 . 2 14
;
; so :
spawn,"sed 's/^.........../ /' fort.14 > f14"
if nmlist eq 0 then spawn,'cat fort.12 f14 | sort -n -k 3,3 >| f12' $
else begin
spawn,"sed 's/^\(..............\)\(...\) /\1 \2 ./' fort.15 > f15"
spawn,'cat fort.12 f15 | sort -n -k 3,3 >| f12'
endelse
lineid_select,'f12',wli,lid,wst,st,ew,ewlim=ewl,range=ra
if n_elements(rv) eq 1 and n_elements(lidshift) ne 0 then $
wli=wli*(1.+rv/2.9977925e5)
if keyword_set(e) then begin
dum=where(strpos(tag_names(e),'CO') ne -1)
if dum ne -1 then dum=e.(dum) else dum=!p.color
endif
lineid_annot,wla,fla,wli,ew,lid,wst,charsize=charsize,extend=extend,col=dum
set_viewport
endif
;
; save files (if parameter SAVE is set)
;
if n_elements(save) eq 1 then begin
a='/bin/mv fort.7 '+save+".7"
spawn,a
a='/bin/mv fort.17 '+save+".17"
spawn,a
a='/bin/mv fort.10 '+save+".10"
spawn,a
a='/bin/mv fort.12 '+save+".12"
spawn,a
a='/bin/mv fort.14 '+save+".14"
spawn,a
a='/bin/mv fort.16 '+save+".16"
spawn,a
a='/bin/mv sylog.tmp '+save+".log"
spawn,a
if n_elements(molecules) gt 0 then begin
a='/bin/mv fort.15 '+save+".15"
spawn,a
endif
if keyword_set(nlte) then begin
a='/bin/mv fort.11 '+save+".11"
spawn,a
endif
; if n_elements(nangles) gt 0 then begin
; a='/bin/mv fort.10 '+save+".int"
; spawn,a
; a='/bin/mv fort.18 '+save+".contint"
; spawn,a
; endif
endif
;
;delete fort.10 if is eq to fort.7
;
;spawn,'/bin/diff fort.7 fort.10',kas
;if strjoin(kas) eq '' then spawn,'/bin/rm -f fort.10'
;
;delete link to fort.19 (line list)
;
if n_elements(linlist) eq 1 then begin
if linlist ne 'fort.19' then begin
; spawn,'/bin/rm -f fort.19'
endif
endif
;
;delete link to fort.20; fort.21; fort.22 (line broadening)
;
;if n_elements(hydprf) eq 1 then begin
; if hydprf ne 'fort.20' then begin
;; spawn,'/bin/rm -f fort.20'
; endif
;endif
;if n_elements(he1prf) eq 1 then begin
; if he1prf ne 'fort.21' then begin
;; spawn,'/bin/rm -f fort.21'
; endif
;endif
;if n_elements(he2prf) eq 1 then begin
; if he2prf ne 'fort.22' then begin
;; spawn,'/bin/rm -f fort.22'
; endif
;endif
;
end
pro rotin,fin,fcont,fout,xout,yout,vrot=vrot,chard=chard,stepr=stepr,$
fwhm=fwhm,stepi=stepi,vmac=vmac,$
wstart=alam0,wend=alam1,relative=irel,help=help
if n_params() lt 3 then begin
print,'rotin,fin,fcont,fout[xout,yout,vrot=,chard=,stepr=,fwhm=,stepi=,vmac=,wstart=,wend=,/relative]'
if ~keyword_set(help) then return
print,' fin : file with synthetic spectrum (.7)'
print,' fcont : file with continuum flux (.17)'
print,' fout : name of the output file'
print,' xout,yout : read fout and store x and y'
print,' VROT - v sin i (in km/s, 0)'
print,' CHARD - characteristic delta lambda (0.01)'
print,' STEPR - wavelength step for evaluation rotational convolution'
print,' FWHM - full width at half maximum instrumental profile'
print,' STEPI - wavelength step for evaluating instrumental convolution '
print,' VMAC - macroturbulent velocity'
print,' ALAM0 - initial wavelength'
print,' ALAM1 - final wavelength'
print,' /RELATIVE - normalized spectrum '
return
endif
spawn,'uname',opsys
; check OS
opsys=strlowcase(strtrim(opsys,2))
case opsys of
'linux' : begin
rotin='./rotin.linux'
end
'darwin': begin
rotin='./rotin.mac'
end
else: begin
message,'# WARNING: I am not sure the OS you are running me on... ',/cont
return
end
endcase
if n_elements(vrot) eq 0 then vrot=0
if n_elements(chard) eq 0 then chard=0
if n_elements(stepr) eq 0 then stepr=0
if n_elements(fwhm) eq 0 then fwhm=0
if n_elements(stepi) eq 0 then stepi=0
if n_elements(vmac) eq 0 then vmac=0
if n_elements(alam0) eq 0 or n_elements(alam1) eq 0 then begin
readcol,fcont,x,/silent
alam0=min(x)
alam1=max(x)
endif
if keyword_set(irel) then irel=1 else irel=0
; ---------------------------------------------------------------
; INPUT - from unit 5 - four lines of input
; ---------------------------------------------------------------
;
; 1. filenames:
;
; fin - name of the file containing the detailed synthetic spectrum
; (i.e. fort.7 produced by Synspec )
;
; fcont - name of the file containing the continuum flux
; (i.e. fort.17 produced by Synspec )
;
; fout - name of the output file - convolved spectrum
;
;
; 2. parameters for rotational convolution
;
; VROT - v sin i (in km/s)
; if VROT=0 - rotational convolution is
; a) either not calculated,
; b) or, if simultaneously FWHM is rather large
; (vrot/c*lambda < FWHM/20.),
; vrot is set to FWHM/20*c/lambda;
; if VROT >0 but the previous condition b) applies, the
; value of VROT is changed as in the previous case
; if VROT<0 - the value of abs(VROT) is used regardless of
; how small compared to FWHM it is
; CHARD - characteristic scale of the variations of unconvolved
; stellar spectrum (basically, characteristic distance
; between two neighbouring wavelength points) - in A
; - if =0 - program sets up default (0.01 A)
; STEPR - wavelength step for evaluation rotational convolution;
; - if =0, the program sets up default (the wavelength
; interval corresponding to the rotational velocity
; devided by 3.)
; if <0, convolved spectrum calculated on the original
; (detailed) SYNSPEC wavelength mesh
;
;
; 3. parameters for instrumental convolution
;
; FWHM - full width at half maximum for Gaussian instrumental
; profile
; STEPI - wavelength step for evaluating instrumental convolution
; - if =0, the program sets up default (FWHM/10.)
; - if <0, convolved spectrum calculated with the previous
; wavelength mesh:
; either the original (SYNSPEC) one if vrot=0,
; or the one used in rotational convolution (vrot > 0)
;
; VMAC - macroturbulent velocity
;
; 4. wavelength interval and normalization of spectra
;
; ALAM0 - initial wavelength
; ALAM1 - final wavelength
; IREL - for =1 relative spectrum
; =0 absolute spectrum
;
openw,1,'rotin3.inp'
printf,1," '",fin,"' '",fcont,"' '",fout,"' "
printf,1,vrot,chard,stepr
printf,1,fwhm,stepi,vmac
printf,1,alam0,alam1,irel
close,1
spawn,rotin+' <rotin3.inp > '+fout+'.log'
if n_params() eq 5 then readcol,fout,xout,yout,/silent,format='(d,d)'
return
end
pro mkintfiles,fort,nmu,muind,fileout,mkcont=mkcont
; fort.10 has the syntetic intensities at different mu
; fort.18 has the continuum intensities at different mu
; nmu = number of mu values
; muind = index(ces) of the mu value to extract (start with 0 i.e.,
; disk centre mu=1.0)
; /mkcont = only make continuum
cc=2.99792458d18 ; speed of light in AA/sec
if ~keyword_set(mkcont) then begin
openr,lun,fort+'.10',/get_lun
lwave=''
lint=''
readf,lun,lwave
kas=strsplit(lwave,' ',/extract)
wave=double(kas[0])
readf,lun,lint
kas=strsplit(lint,' ',/extract)
nread=0
while n_elements(kas) lt nmu do begin
readf,lun,lint
nread++
kas=[kas,strsplit(lint,' ',/extract)]
endwhile
int=double(kas)
while(~eof(lun)) do begin
readf,lun,lwave
readf,lun,lint
kas=strsplit(lwave,' ',/extract)
wave=[wave,double(kas[0])]
kas=strsplit(lint,' ',/extract)
for jj=1, nread do begin
readf,lun,lint
kas=[kas,strsplit(lint,' ',/extract)]
endfor
int=[[int],[double(kas)]]
endwhile
close,lun
openw,lun,fileout+'.int'
for ii=0, n_elements(wave)-1 do printf,lun,wave[ii],int[muind,ii]*cc/wave[ii]/wave[ii],format='(f12.5,e15.5E3)'
close,lun
endif else get_lun,lun
;;; fort.18 continuum intensity
openr,lun,fort+'.18'
lwave=''
lint=''
readf,lun,lwave
kas=strsplit(lwave,' ',/extract)
wave=double(kas[0])
readf,lun,lint
kas=strsplit(lint,' ',/extract)
nread=0
while n_elements(kas) lt nmu do begin
readf,lun,lint
nread++
kas=[kas,strsplit(lint,' ',/extract)]
endwhile
int=double(kas)
while(~eof(lun)) do begin
readf,lun,lwave
kas=strsplit(lwave,' ',/extract)
wave=[wave,double(kas[0])]
readf,lun,lint
kas=strsplit(lint,' ',/extract)
for jj=1, nread do begin
readf,lun,lint
kas=[kas,strsplit(lint,' ',/extract)]
endfor
int=[[int],[double(kas)]]
endwhile
close,lun
openw,lun,fileout+'.contint'
for ii=0, n_elements(wave)-1 do if (ii mod 4 eq 2) or (ii mod 4 eq 3) then printf,lun,wave[ii],int[muind,ii]*cc/wave[ii]/wave[ii],format='(f12.5,e15.5E3)'
; for ii=0, n_elements(wave)-1 do printf,lun,wave[ii],int[muind,ii]*cc/wave[ii]/wave[ii],format='(f12.5,e15.5E3)'
close,lun
free_lun,lun
end
+106
View File
@@ -0,0 +1,106 @@
def opa(file,indt=0,indr=0):
import matplotlib.pyplot as plt
import numpy as np
import sys
try:
f = open(file)
lines = f.readlines()
except:
print('Error: Could not open %s' % modfile)
return()
ntrow = 6
i = 40
x=lines[i]
nfre = int(x.split()[0])
ntem = int(x.split()[1])
nrho = int(x.split()[2])
print(nfre,ntem,nrho)
i = i+2
nreat = ntem//ntrow
if ntem % ntrow != 0:
nreat = nreat + 1
temp = []
j = 0
while j < nreat:
x = lines[i]
val = x.split()
k = 0
while k < ntrow:
if (j*ntrow + k) < ntem:
temp.append(float(val[k]))
k+= 1
j+= 1
i+= 1
print(np.exp(temp))
i+= 1
nrear = nrho//ntrow
if nrho % ntrow != 0:
nrear = nrear + 1
dens = []
j = 0
while j < nrear:
x = lines[i]
val = x.split()
k = 0
while k < ntrow:
if (j*ntrow + k) < nrho:
dens.append(float(val[k]))
k+= 1
j+= 1
i+= 1
i+= 1
print(np.exp(dens))
nl = ntem*nrho
nrel = nl//ntrow
if nl % ntrow != 0:
nrel = nrel + 1
i=i+nrel
lamb=[]
abso=[]
ilam = 0
while ilam < nfre:
i+= 1
x = lines[i]
val = x.split()
lamb.append(float(val[5]))
i = i+2
it = 0
ir = 0
while ir < nrho:
j = 0
abt=[]
while j < nreat:
x = lines[i]
val = x.split()
k = 0
while k < ntrow:
if(j*ntrow + k) < ntem:
abt.append(float(val[k]))
k+=1
j+=1
i+=1
if ir == indr:
abso.append(abt[indt])
ir+=1
ilam += 1
lamb = np.array(lamb)
abso = np.array(abso)
print(ilam)
return(lamb,abso)
+192
View File
@@ -0,0 +1,192 @@
pro pconv,datfile,relcfile,timfile,hc,notemp=notemp
;
;plots the convergence log (from unit 9) for stellar atmospheres
; (output from TLUSTY), as well as disks (TLUSDIDK).
;
;datfile, relcfile - names for units 7 and 9 outputs, respectively:
;if RELCFILE is missing, and only DATFILE is present, then the program
; assumes that the names are: DATFILE.7 and DATFILE.9 (i.e. the parameter
; DATFILE contains the core of the name, without any extensions);
;if both are present, they contains the names in full (useful for owerwriting
; the standard notation convention);
;if both are absent, the program assumes the names being: fort.7 and fort.9;
;
;use hc for hardcopy (0=default, 6=portrait,5=landscape)
;use ymin and ymax to override default y-axis limits
if n_params(0) lt 4 then hc=0
if n_params(0) eq 1 then begin
datf=datfile+'.7'
relcfile=datfile+'.9'
timfile=datfile+'.69'
datfile=datf
endif
if n_params(0) eq 0 then begin
datfile='fort.7'
relcfile='fort.9'
timfile='fort.69'
endif
;GET MASS DEPTH ARRAY, NITER, ND
get_lun,lun
a=''
openr,lun,datfile
data=intarr(2)
readf,lun,data
nd=data(0)
mass=fltarr(nd)
readf,lun,mass
free_lun,lun
get_lun,lun
openr,lun,relcfile
CT=FLTARR(ND,200) & CP=CT & CNE=CT & CMAX=CT ;DEFINE OUTPUT ARRAYS
tmax=fltarr(200) & mmax=tmax & itrn=tmax
for i=1,3 do readf,lun,a ;skip 3 lines
data=fltarr(9)
k=-1
while not eof(lun) do begin
k=k+1
for j=1,nd do begin
readf,lun,data
ct(j-1,k)=data(2)
cp(j-1,k)=data(4)
cne(j-1,k)=data(3)
cmax(j-1,k)=data(6)
end
endwhile
niter=k+1 ;actual number of iterations
if niter eq 1 then ct=fltarr(nd,1)+ct(*,0) else ct=ct(*,0:k)
if niter eq 1 then cp=fltarr(nd,1)+cp(*,0) else cp=cp(*,0:k)
if niter eq 1 then cne=fltarr(nd,1)+cne(*,0) else cne=cne(*,0:k)
if niter eq 1 then cmax=fltarr(nd,1)+cmax(*,0) else cmax=cmax(*,0:k)
;REVERSE TO AGREE WITH MASS DEPTH COORDINATE
for k=0,niter-1 do begin
;ct(0,k)=reverse(ct(*,k))
;cp(0,k)=reverse(cp(*,k))
;cne(0,k)=reverse(cne(*,k))
;cmax(0,k)=reverse(cmax(*,k))
end
if n_elements(notemp) eq 0 then lct=alog10(abs(ct))
lcmax=alog10(abs(cmax))
for k=0,niter-1 do begin
if n_elements(notemp) eq 0 then tmax(k)=max(lct(*,k))
mmax(k)=max(lcmax(*,k))
itrn(k)=k+1.
end
free_lun,lun
ITER=STRTRIM(NITER,2)
x=alog10(mass)
!xtitle='Log Depth (Mass)
if hc ne 0 then set_plot,'ps'
if hc eq 6 then device,/landscape
!p.multi=[0,3,2]
;1st plot
if n_elements(notemp) eq 0 then begin
;set_viewport,.15,.38,.575,.875
;!mtitle='Temperature
!ytitle='Relative Change
plot,x,ct(*,0),yrange=[min(ct),max(ct)]
if niter gt 1 then for k=1,niter-1 do oplot,x,ct(*,k),line=k
;!noeras=1
endif
;2nd plot
if n_elements(notemp) eq 0 then begin
;set_viewport,.44,.67,.575,.875
!ytitle=''
yt='Log !9!!!3 Relative Change !9!!!3'
plot,x,lct(*,0),yrange=[min(lct),max(lct)]
if niter gt 1 then for k=1,niter-1 do oplot,x,lct(*,k),line=k
endif
;3rd plot
; set_viewport,.15,.38,.15,.45
;!mtitle='Maximum in State Vector
!ytitle='Relative Change
plot,x,cmax(*,0),yrange=[min(cmax),max(cmax)]
if niter gt 1 then for k=1,niter-1 do oplot,x,cmax(*,k),line=k
;!noeras=1
;4th plot
;set_viewport,.44,.67,.15,.45
;!mtitle='Maximum in State Vector
!ytitle=''
yt='Log !9!!!3 Relative Change !9!!!3'
plot,x,lcmax(*,0),yrange=[min(lcmax),max(lcmax)]
if niter gt 1 then for k=1,niter-1 do oplot,x,lcmax(*,k),line=k
;5th plot
if n_elements(notemp) eq 0 then begin
;set_viewport,.73,.96,.575,.875
;!mtitle='Temperature
;!xtitle='iteration'
!ytitle=''
yt='Log !9!!!3 Relative Change !9!!!3'
plot,itrn(0:niter-1),tmax(0:niter-1),psym=-1
endif
;6th plot
;set_viewport,.73,.96,.15,.45
;!mtitle='Maximum in State Vector
;!xtitle='iteration'
!ytitle=''
yt='Log !9!!!3 Relative Change !9!!!3'
plot,itrn(0:niter-1),mmax(0:niter-1),psym=-1
;
tit=relcfile
spawn,'rm -f tmp'
spawn,'date >tmp'
close,2
openr,2,'tmp'
a=''
readf,2,a
if hc eq 0 then xyouts,0.8,0.98,a,/normal else $
xyouts,0.8,0.98,a,/normal,size=0.5
close,2
spawn,'rm -f tmp'
;xyouts,0.5,0.98,tit,alignment=0.5,size=2,/normal
;
!p.multi=0
!p.title=''
;!noeras=0
!xtitle=''
;set_viewport
;
openr,2,timfile
while not eof(2) do readf,2,t1,t2,t3
tit=tit+' time='+strcompress(string(format='(i)',(t3)))+' sec'
xyouts,0.5,0.92,tit,alignment=0.5,size=2,/normal
close,2
;
if hc ne 0 then begin
device,/close
set_plot,'x'
spawn,'mac_ps idl.ps'
; spawn,'rm -f idl.ps'
end
return
end
+149
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@@ -0,0 +1,149 @@
pro pmodels,files,ipar,mode,ipl,hc, $
colbeg=colbeg,colstep=colstep,nohead=nohead,_extra=e
;
; plots the output from Tlusty or Tlusdisk - unit 7 (*.card file)
; files - filename(s)
; ipar - model quantity to be plotted (0=temperature; 1=electron density;
; 2=density; 3= first population; 2+i = i-th population);
; Note: in case of disks; ipar=3 plots z(m)
; mode = 0 - absolute value(s) (logarithms for number densities);
; = 1 - differences; the first file is the reference one);
; ipl = 0 - plot
; = 1 - overplot
; hc = 0 - plot appears on screen
; > 0 - the run generates an idl.ps file to be printed on a postscript
; printer
common modpar,t,dt,dm,dml,dm0,temp0,tmi,tit,x
;
if n_params(0) le 4 then hc=0
if n_params(0) le 3 then ipl=0
if n_params(0) le 2 then mode=0
if n_params(0) le 1 then ipar=0
;
if n_elements(colbeg) eq 0 then colbeg=40
if n_elements(colstep) eq 0 then colstep=15
s=size(files)
nmod=s(1)
f=strarr(nmod)
!ignore=0
;
if hc gt 0 then begin
set_plot,'ps'
device,/landscape
endif
;
; set up the plot title (list of files)
;
tit=''
for ip=0,nmod-1 do begin
if strpos(files(ip),'.') gt -1 then f(ip)=files(ip) else f(ip)=files(ip)+'.7'
tit=tit+files(ip)
if ip lt nmod-1 then tit=tit+','
endfor
;
; set up title for y-axis
;
yt=''
if mode eq 0 then begin
if ipar eq 0 then yt='temperature'
if ipar eq 1 then yt='log n(e)'
if ipar eq 2 then yt='log density'
endif
if mode eq 1 then begin
if ipar eq 0 then yt='Delta T'
if ipar eq 1 then yt='Delta log n(e)'
if ipar eq 2 then yt='Delta log density'
endif
; read first model
;
get_lun,l1
openr,l1,f(0)
readf,l1,nd,np
dm=fltarr(nd)
x=fltarr(np,nd)
readf,l1,dm
readf,l1,x
dml=alog10(dm)
if ipar eq 0 then t=x(0,*) else t=alog10(x(ipar,*))
if mode eq 1 then begin
dm0=dml
temp0=t
dt0=t-temp0
endif
free_lun,l1
; plot first model
;
if mode eq 0 then begin
if ipl eq 0 then plot,dml,t,xtit='log mass',ytit=yt,_extra=e else oplot,dml,t
endif
;
; read and plot next models
;
if nmod ge 1 then begin
for ip=1,nmod-1 do begin
get_lun,l1
openr,l1,f(ip)
readf,l1,nd,np
dm=fltarr(nd)
x=fltarr(np,nd)
readf,l1,dm
readf,l1,x
dml=alog10(dm)
if ipar eq 0 then t=x(0,*) else t=alog10(x(ipar,*))
if mode eq 1 then begin
dml=alog10(dm)
tmi=interpol(t,dml,dm0)
dt=tmi-temp0
if ip eq 1 then if ipl eq 0 then $
plot,dm0,dt,psym=3,xtit='log mass',ytit=yt,_extra=e $
else oplot,dm0,dt
endif
free_lun,l1
if hc eq 0 then begin
co=ip*20+100
co=colbeg+colstep*ip
li=0
endif else begin
co=0
li=ip
endelse
;
if mode eq 0 then oplot,dml,t,color=co,line=li else $
oplot,dm0,dt,color=co,line=li
endfor
endif
if mode eq 1 then oplot,dm0,dt0
;
if n_elements(nohead) eq 0 then begin
if ipl eq 0 then begin
spawn,'date >tmp'
openr,2,'tmp'
a=''
readf,2,a
if hc eq 0 then xyouts,0.8,0.98,a,/normal else $
xyouts,0.8,0.98,a,/normal,size=0.5
close,2
spawn,'rm -f tmp'
xyouts,0.5,0.98,tit,alignment=0.5,size=2,/normal
endif
endif
;
if hc gt 0 then begin
device,/close
spawn,'mac_ps idl.ps'
set_plot,'x'
endif
;
return
end
+4
View File
@@ -0,0 +1,4 @@
linelists/*19*
linelists/*20*
bin/s*
bin/rotin*
+19
View File
@@ -0,0 +1,19 @@
Copyright (c) 2020 callendeprieto
Permission is hereby granted, free of charge, to any person obtaining a copy
of this software and associated documentation files (the "Software"), to deal
in the Software without restriction, including without limitation the rights
to use, copy, modify, merge, publish, distribute, sublicense, and/or sell
copies of the Software, and to permit persons to whom the Software is
furnished to do so, subject to the following conditions:
The above copyright notice and this permission notice shall be included in all
copies or substantial portions of the Software.
THE SOFTWARE IS PROVIDED "AS IS", WITHOUT WARRANTY OF ANY KIND, EXPRESS OR
IMPLIED, INCLUDING BUT NOT LIMITED TO THE WARRANTIES OF MERCHANTABILITY,
FITNESS FOR A PARTICULAR PURPOSE AND NONINFRINGEMENT. IN NO EVENT SHALL THE
AUTHORS OR COPYRIGHT HOLDERS BE LIABLE FOR ANY CLAIM, DAMAGES OR OTHER
LIABILITY, WHETHER IN AN ACTION OF CONTRACT, TORT OR OTHERWISE, ARISING FROM,
OUT OF OR IN CONNECTION WITH THE SOFTWARE OR THE USE OR OTHER DEALINGS IN THE
SOFTWARE.
+56
View File
@@ -0,0 +1,56 @@
# synple
An Easy-to-Use Python Wrapper for the Spectral Synthesis Code Synspec
** install **
Starting in the main synple directory
1- Compile synspec and rotin
Make sure you have a fortran compiler -- gfortran, is expected and
if you are using a different compiler you will need to modify the
makefile accordingly.
cd synspec
make clean; make
cd ..
2- Download the line list data
Make sure you have wget and a working internet connection
cd linelists
make clean; make
cd ..
3- Add the synple directory to your $PYTHONPATH enviromental variable (optional)
4- Make sure you have a working python install!
** test **
Copy one of the model atmospheres in the 'models' folder (e.g. to your working
directory) and test that the code works. For example if you use the MARCS model
sun.mod and want to compute the solar spectrum between 6160. and 6164. AA
synple.py sun.mod 6160. 6164.
or, similarly, from a python interpreter (e.g. ipython)
from synple import syn
x, y, z = syn('ksun.mod', (6160.,6164.))
#and to plot the continuum normalized spectrum
%pylab
plot(x,y/z)
+26
View File
@@ -0,0 +1,26 @@
#
# makefile for downloading synple/synspec line lists
# Carlos 2019
#
FTP = ftp://carlos:allende@ftp.ll.iac.es/atlases/
WGET = `which wget`
#general line lists
STANDARD = ardata.fits iag-nir.fits iag-vis.fits solarfluxintwl.fits ardata-ReadMe.txt iag-ReadMe.txt solarfluxintwl-ReadMe.txt
#STANDARD = solarfluxintwl.fits solarfluxintwl-ReadMe.txt
all:
$(call sequence, $(STANDARD))
clean:
rm -f *.fits *.txt
define sequence
for file in $(1) ; do \
${WGET} ${FTP}$$file ; \
done
endef
Binary file not shown.
+39
View File
@@ -0,0 +1,39 @@
wrange: 2000. 30000.
vmicro: -1
grids: ['f_dr16-apo1','f_dr16-apo2','f_dr16-apo3','f_dr16-apo4','f_dr16-apo5']
f_dr16-apo1:
type: 'marcs'
tteff: 11 3500. 250.
tlogg: 10 0.0 0.5
tfeh: 15 -2.5 0.25
tafe: 8 -0.75 0.25
tcfe: 11 -1.50 0.25
f_dr16-apo2:
type: 'marcs'
tteff: 11 3000. 100.
tlogg: 8 -0.5 0.5
tfeh: 15 -2.5 0.25
tafe: 8 -0.75 0.25
tcfe: 11 -1.50 0.25
f_dr16-apo3:
type: 'marcs'
tteff: 11 5500. 250.
tlogg: 7 2.5 0.5
tfeh: 15 -2.5 0.25
tafe: 8 -0.75 0.25
tcfe: 5 -0.50 0.25
f_dr16-apo4:
type: 'marcs'
tteff: 11 3500. 250.
tlogg: 7 2.5 0.5
tfeh: 15 -2.5 0.25
tafe: 8 -0.75 0.25
tcfe: 5 -0.50 0.25
f_dr16-apo5:
type: 'marcs'
tteff: 11 3000. 100.
tlogg: 7 2.5 0.5
tfeh: 15 -2.5 0.25
tafe: 8 -0.75 0.25
tcfe: 5 -0.50 0.25
+92
View File
@@ -0,0 +1,92 @@
STIS:
gsynth: [
{'fwhm': 600., 'units': 'km/s', 'ppr': 3., 'wrange': [3000.,9900.],
'outsynthfile': 'n_STIS.dat' }]
bas_perfcheck: [
{'synthfile': 'n_STIS.dat'},
{'synthfile': 'n_STIS.dat', 'snr' : 30 },
{'synthfile': 'n_STIS.dat', 'snr' : 10 } ]
pickle_synth: [
{'synthfile': 'n_STIS.dat'} ]
STIS-NICMOS:
gsynth: [
{'fwhm': 600., 'units': 'km/s', 'ppr': 3., 'wrange': [3000.,29900.],
'outsynthfile': 'n_STIS-NICMOS.dat' }]
bas_perfcheck: [
{'synthfile': 'n_STIS-NICMOS.dat'},
{'synthfile': 'n_STIS-NICMOS.dat', 'snr' : 30 },
{'synthfile': 'n_STIS-NICMOS.dat', 'snr' : 10 } ]
pickle_synth: [
{'synthfile': 'n_STIS-NICMOS.dat'} ]
MILES:
gsynth: [
{'fwhm': 2.5, 'units': 'A', 'ppr': 3., 'wrange': [3510.,7400.],
'outsynthfile': 'n_MILES.dat' }]
bas_perfcheck: [
{'synthfile': 'n_MILES.dat'},
{'synthfile': 'n_MILES.dat', 'snr' : 30 },
{'synthfile': 'n_MILES.dat', 'snr' : 10 } ]
pickle_synth: [
{'synthfile': 'n_MILES.dat'} ]
IDS-R900V:
gsynth: [
{'fwhm': 1.89, 'units': 'A', 'ppr': 3., 'wrange': [3760.,5180.],
'outsynthfile': 'n_IDS-R900V.dat' }]
bas_perfcheck: [
{'synthfile': 'n_IDS-R900V.dat'},
{'synthfile': 'n_IDS-R900V.dat', 'snr' : 30 },
{'synthfile': 'n_IDS-R900V.dat', 'snr' : 10 } ]
pickle_synth: [
{'synthfile': 'n_IDS-R900V.dat'} ]
OSIRIS-R2500U:
gsynth: [
{'fwhm': 1.55, 'units': 'A', 'ppr': 3., 'wrange': [3500.,4600.],
'outsynthfile': 'n_OSIRIS-R2500U.dat' }]
bas_perfcheck: [
{'synthfile': 'n_OSIRIS-R2500U.dat'},
{'synthfile': 'n_OSIRIS-R2500U.dat', 'snr' : 30 },
{'synthfile': 'n_OSIRIS-R2500U.dat', 'snr' : 10 } ]
pickle_synth: [
{'synthfile': 'n_OSIRIS-R2500U.dat'} ]
XP:
gsynth: [
{'fwhm': 299.792458, 'units': 'km/s', 'ppr': 3., 'wrange':[3000., 11000.],
'outsynthfile': 'n_R1000.dat'} ]
xplsf: [
{'synthfile': 'i_R1000.dat', 'outsynthfile': 'v_XP.dat'} ]
bas_perfcheck: [
{'synthfile': 'v_XP.dat'},
{'synthfile': 'v_XP.dat', 'snr' : 30 },
{'synthfile': 'v_XP.dat', 'snr' : 10 } ]
pickle_synth: [
{'synthfile': 'v_XP.dat'} ]
LAMOST:
gsynth: [
{'fwhm':167., 'units':'km/s', 'ppr':3., 'wrange':[3800., 9000.],
'outsynthfile': 'n_LAMOST.dat'} ]
bas_perfcheck: [
{'synthfile': 'n_LAMOST.dat'},
{'synthfile': 'n_LAMOST.dat', 'snr': 30 },
{'synthfile': 'n_LAMOST.dat', 'snr': 10 } ]
pickle_synth: [
{'synthfile': 'n_LAMOST.dat'} ]
DESI:
gsynth: [
{'fwhm': 1.8, 'units': 'A', 'ppr': 3., 'wrange': [3759., 5959],
'outsynthfile': 'n_B-DESI.dat'},
{'fwhm': 1.8, 'units': 'A', 'ppr': 3., 'wrange': [5635., 7750.],
'outsynthfile': 'n_R-DESI.dat'},
{'fwhm': 1.8, 'units': 'A', 'ppr': 3., 'wrange': [7445., 9843.],
'outsynthfile': 'n_Z-DESI.dat'} ]
paste_synth: [
{'synthfile': ['n_B-DESI.dat','n_R-DESI.dat','n_Z-DESI.dat'],
'outsynthfile': 'n_BRZ-DESI.dat'} ]
synth_rbf: [
{'synthfile': 'n_BRZ-DESI.dat',
'n': 10000, 'rv': False, 'ebv': False} ]
bas_perfcheck: [
{'synthfile': 'n_BRZ-DESI.dat'},
{'synthfile': 'n_BRZ-DESI.dat', 'snr': 30 },
{'synthfile': 'n_BRZ-DESI.dat', 'snr': 10 } ]
pickle_synth: [
{'synthfile': 'n_BRZ-DESI.dat'} ]
+161
View File
@@ -0,0 +1,161 @@
STIS:
gsynth: [
{'fwhm': 600., 'units': 'km/s', 'ppr': 3., 'wrange': [3000.,9900.],
'outsynthfile': 'n_STIS.dat' }]
rewrite_synth: [
{'synthfile': 'n_STIS.dat', 'outsynthfile': 'i_STIS.dat'}]
synth_rbf: [
{'synthfile': 'i_STIS.dat',
'n': 10000, 'rv': False, 'ebv': False},
{'synthfile': 'i_STIS.dat',
'n': 10000, 'rv': False, 'ebv': True} ]
bas_perfcheck: [
{'synthfile': 'n_STISrbf.dat'},
{'synthfile': 'n_STISrbf.dat', 'snr' : 30 },
{'synthfile': 'n_STISrbf.dat', 'snr' : 10 },
{'synthfile': 'n_STISrbf-EBV.dat'},
{'synthfile': 'n_STISrbf-EBV.dat', 'snr' : 30 },
{'synthfile': 'n_STISrbf-EBV.dat', 'snr' : 10 } ]
pickle_synth: [
{'synthfile': 'n_STISrbf.dat'},
{'synthfile': 'n_STISrbf-EBV.dat'} ]
STIS-NICMOS:
gsynth: [
{'fwhm': 600., 'units': 'km/s', 'ppr': 3., 'wrange': [3000.,29900.],
'outsynthfile': 'n_STIS-NICMOS.dat' }]
rewrite_synth: [
{'synthfile': 'n_STIS-NICMOS.dat', 'outsynthfile': 'i_STIS-NICMOS.dat'}]
synth_rbf: [
{'synthfile': 'i_STIS-NICMOS.dat',
'n': 10000, 'rv': False, 'ebv': False},
{'synthfile': 'i_STIS-NICMOS.dat',
'n': 10000, 'rv': False, 'ebv': True} ]
bas_perfcheck: [
{'synthfile': 'n_STIS-NICMOSrbf.dat'},
{'synthfile': 'n_STIS-NICMOSrbf.dat', 'snr' : 30 },
{'synthfile': 'n_STIS-NICMOSrbf.dat', 'snr' : 10 },
{'synthfile': 'n_STIS-NICMOSrbf-EBV.dat'},
{'synthfile': 'n_STIS-NICMOSrbf-EBV.dat', 'snr' : 30 },
{'synthfile': 'n_STIS-NICMOSrbf-EBV.dat', 'snr' : 10 } ]
pickle_synth: [
{'synthfile': 'n_STIS-NICMOSrbf.dat'},
{'synthfile': 'n_STIS-NICMOSrbf-EBV.dat'} ]
MILES:
gsynth: [
{'fwhm': 2.5, 'units': 'A', 'ppr': 3., 'wrange': [3510.,7400.],
'outsynthfile': 'n_MILES.dat' }]
rewrite_synth: [
{'synthfile': 'n_MILES.dat', 'outsynthfile': 'i_MILES.dat'}]
synth_rbf: [
{'synthfile': 'i_MILES.dat',
'n': 10000, 'rv': False, 'ebv': False} ]
bas_perfcheck: [
{'synthfile': 'n_MILESrbf.dat'},
{'synthfile': 'n_MILESrbf.dat', 'snr' : 30 },
{'synthfile': 'n_MILESrbf.dat', 'snr' : 10 } ]
pickle_synth: [
{'synthfile': 'n_MILESrbf.dat'} ]
IDS-R900V:
gsynth: [
{'fwhm': 1.89, 'units': 'A', 'ppr': 3., 'wrange': [3760.,5180.],
'outsynthfile': 'n_IDS-R900V.dat' }]
rewrite_synth: [
{'synthfile': 'n_IDS-R900V.dat', 'outsynthfile': 'i_IDS-R900V.dat'}]
synth_rbf: [
{'synthfile': 'i_IDS-R900V.dat',
'n': 10000, 'rv': False, 'ebv': False} ]
bas_perfcheck: [
{'synthfile': 'n_IDS-R900Vrbf.dat'},
{'synthfile': 'n_IDS-R900Vrbf.dat', 'snr' : 30 },
{'synthfile': 'n_IDS-R900Vrbf.dat', 'snr' : 10 } ]
pickle_synth: [
{'synthfile': 'n_IDS-R900Vrbf.dat'} ]
OSIRIS-R2500U:
gsynth: [
{'fwhm': 1.55, 'units': 'A', 'ppr': 3., 'wrange': [3500.,4600.],
'outsynthfile': 'n_OSIRIS-R2500U.dat' }]
rewrite_synth: [
{'synthfile': 'n_OSIRIS-R2500U.dat', 'outsynthfile': 'i_OSIRIS-R2500U.dat'}]
synth_rbf: [
{'synthfile': 'i_OSIRIS-R2500U.dat',
'n': 10000, 'rv': False, 'ebv': False} ]
bas_perfcheck: [
{'synthfile': 'n_OSIRIS-R2500Urbf.dat'},
{'synthfile': 'n_OSIRIS-R2500Urbf.dat', 'snr' : 30 },
{'synthfile': 'n_OSIRIS-R2500Urbf.dat', 'snr' : 10 } ]
pickle_synth: [
{'synthfile': 'n_OSIRIS-R2500Urbf.dat'} ]
XP:
gsynth: [
{'fwhm': 299.792458, 'units': 'km/s', 'ppr': 3., 'wrange':[3000., 11000.],
'outsynthfile': 'n_R1000.dat'} ]
rewrite_synth: [
{'synthfile': 'n_R1000.dat', 'outsynthfile': 'i_R1000.dat'}]
xplsf: [
{'synthfile': 'i_R1000.dat', 'outsynthfile': 'v_XP.dat'} ]
synth_rbf: [
{'synthfile': 'v_XP.dat',
'n': 10000, 'rv': False, 'ebv': False},
{'synthfile': 'v_XP.dat',
'n': 10000, 'rv': False, 'ebv': True} ]
bas_perfcheck: [
{'synthfile': 'n_XPrbf.dat'},
{'synthfile': 'n_XPrbf.dat', 'snr' : 30 },
{'synthfile': 'n_XPrbf.dat', 'snr' : 10 },
{'synthfile': 'n_XPrbf-EBV.dat'},
{'synthfile': 'n_XPrbf-EBV.dat', 'snr': 30 },
{'synthfile': 'n_XPrbf-EBV.dat', 'snr': 10 } ]
pickle_synth: [
{'synthfile': 'n_XPrbf.dat'},
{'synthfile': 'n_XPrbf-EBV.dat'} ]
LAMOST:
gsynth: [
{'fwhm':167., 'units':'km/s', 'ppr':3., 'wrange':[3800., 9000.],
'outsynthfile': 'n_LAMOST.dat'} ]
rewrite_synth: [
{'synthfile': 'n_LAMOST.dat', 'outsynthfile': 'i_LAMOST.dat'}]
synth_rbf: [
{'synthfile': 'i_LAMOST.dat',
'n': 10000, 'rv': False, 'ebv': False},
{'synthfile': 'i_LAMOST.dat',
'n': 10000, 'rv': False, 'ebv': True} ]
bas_perfcheck: [
{'synthfile': 'n_LAMOSTrbf.dat'},
{'synthfile': 'n_LAMOSTrbf.dat', 'snr': 30 },
{'synthfile': 'n_LAMOSTrbf.dat', 'snr': 10 },
{'synthfile': 'n_LAMOSTrbf-EBV.dat'},
{'synthfile': 'n_LAMOSTrbf-EBV.dat', 'snr': 30 },
{'synthfile': 'n_LAMOSTrbf-EBV.dat', 'snr': 10 } ]
pickle_synth: [
{'synthfile': 'n_LAMOSTrbf.dat'},
{'synthfile': 'n_LAMOSTrbf-EBV.dat'} ]
DESI:
gsynth: [
{'fwhm': 1.8, 'units': 'A', 'ppr': 3., 'wrange': [3759., 5959],
'outsynthfile': 'n_B-DESI.dat'},
{'fwhm': 1.8, 'units': 'A', 'ppr': 3., 'wrange': [5635., 7750.],
'outsynthfile': 'n_R-DESI.dat'},
{'fwhm': 1.8, 'units': 'A', 'ppr': 3., 'wrange': [7445., 9843.],
'outsynthfile': 'n_Z-DESI.dat'} ]
rewrite_synth: [
{'synthfile': 'n_B-DESI.dat', 'outsynthfile': 'i_B-DESI.dat'},
{'synthfile': 'n_R-DESI.dat', 'outsynthfile': 'i_R-DESI.dat'},
{'synthfile': 'n_Z-DESI.dat', 'outsynthfile': 'i_Z-DESI.dat'}]
paste_synth: [
{'synthfile': ['i_B-DESI.dat','i_R-DESI.dat','i_Z-DESI.dat'],
'outsynthfile': 'i_BRZ-DESI.dat'} ]
synth_rbf: [
{'synthfile': 'i_BRZ-DESI.dat',
'n': 10000, 'rv': False, 'ebv': False},
{'synthfile': 'i_BRZ-DESI.dat',
'n': 10000, 'rv': False, 'ebv': True} ]
bas_perfcheck: [
{'synthfile': 'n_BRZ-DESIrbf.dat'},
{'synthfile': 'n_BRZ-DESIrbf.dat', 'snr': 30 },
{'synthfile': 'n_BRZ-DESIrbf.dat', 'snr': 10 },
{'synthfile': 'n_BRZ-DESIrbf-EBV.dat'},
{'synthfile': 'n_BRZ-DESIrbf-EBV.dat', 'snr': 30 },
{'synthfile': 'n_BRZ-DESIrbf-EBV.dat', 'snr': 10 } ]
pickle_synth: [
{'synthfile': 'n_BRZ-DESIrbf.dat'},
{'synthfile': 'n_BRZ-DESIrbf-EBV.dat'} ]
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DESI: n_sc2-BRZ-DESIrbf.pickle
IDS-R900V: n_sc2-IDS-R900Vrbf.pickle
LAMOST: n_sc2-LAMOSTrbf.pickle
MILES: n_sc2-MILESrbf.pickle
OSIRIS-R2500U: n_sc2-OSIRIS-R2500Urbf.pickle
STIS-NICMOS: n_sc2-STIS-NICMOSrbf.pickle
XP: n_sc2-XPrbf.pickle
CALSPEC: n_sc2-STISrbf.pickle
STIS: n_sc2-STISrbf.pickle
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all: synple.pdf
clean:
rm synple.aux synple.dvi synple.log synple.toc synple.pdf
synple.pdf: synple.tex
latex synple.tex
latex synple.tex
dvipdf synple
rm synple.aux synple.dvi synple.log synple.toc
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\documentclass[]{article}
\usepackage{graphicx}
%times,palatino,bookman, palatino, newcent
\usepackage{geometry}
\geometry{ a4paper, total={210mm,297mm},
left=25mm,
right=25mm,
top=20mm,
bottom=20mm,
}
\begin{document}
\title{Synple User's Guide}
\date{\today}
\author{C. Allende Prieto, I. Hubeny, T. Lanz, Y. M. Osorio}
\maketitle
{\tt Synple} is a Python interface to the spectral synthesis code Synspec
and a set of related utilities. Synple can compute emerging spectra from LTE Kurucz,
MARCS, Phoenix or Tlusty model atmospheres, as well as NLTE Tlusty models. Appropriate
default choices for the continuum and line opacities are provided, while the chemical
abundances and micro-turbulence velocity are taken from the input model atmospheres, but
can be changed as needed.
\tableofcontents
\newpage
\section{Introduction}
\label{intro}
The computation of detailed stellar stellar spectra is a basic but important step required for the analysis of star light, spectra of integrated stellar populations, or transiting planets. The calculations involve solving the equation of radiative transfer
\begin{equation}
\cos \theta \frac{d I_{\nu} (\theta)}{dz} = \eta_{\nu} - \kappa_{\nu} I_{\nu} (\theta) + \int_0^{\pi} I_{\nu} (\theta') \phi (\theta') \sin \theta' d\theta',
\end{equation}
\noindent where $I_{\nu}$ is the specific intensity, and describes the radiation field (radiative energy per unit of frequency propagating at an angle $\theta$ from the vertical traversing a unit area per unit time), $\kappa$ is the opacity (fraction of energy absorbed per unit length), $\eta$ the emissivity (energy emited, same units as the intensity) and $\phi$ represents the scattering function (photons scattered from the direction $\theta$' into the direction $\theta$.
Once $I_{\nu}$ ($\theta$) is known, it can be integrated to derive the stellar flux
\begin{equation}
H_{\nu} = \int_0^{\pi} I_{\nu} (\theta) \cos \theta \sin \theta d\theta
\label{flux}
\end{equation}
\noindent which can be finally convolved with various kernels that describe large-scale atmospheric turbulence, rotation, or the instrumental profile.
Prior to solving the equation of radiative transfer, one requires a physical model of the stellar atmosphere in order to compute $\eta$, $\kappa$ and $\phi$. This is the running of the thermodynamical quantities (e.g temperature and density) with height, as well as the chemical composition. This input {\it model atmosphere} is the sole required input to Synple. Of course, computing a detailed spectrum requires fundamental physical data on the interaction of matter and radiation (photoionization cross-sections, atomic and molecular transition probabilities and damping constants, etc), but a generic collection of such data is bundled with Synspec.
Multiple codes for radiative transfer exist and are publicly available. However, most require deep knowledge of the related physics and are cumbersome to use. Synple provides an easy-to-use Python interface to Synspec (Hubeny \& Lanz 2017; Hubeny et al. 2021) for the fast computation of model stellar spectra with accuracy and flexibility.
Note that the quantities returned by Synple are
per unit (vacuum) wavelength, i.e. $H_{\lambda}$ and $I_{\lambda}$,
rather than per unit frequency, $H_{\nu}$ and $I_{\nu}$, but the conversion
is trivial by requiring that $I_{\nu} d\nu = I_{\lambda} d\lambda$
\begin{eqnarray}
H_{\lambda} = \frac{\nu^2}{c} H_{\nu},
I_{\lambda} = \frac{\nu^2}{c} I_{\nu},
\end{eqnarray}
and the returned wavelength arrays are given for standard air
for $\lambda > 2000$ \AA\ and
vacuum otherwise.
\section{Installing}
Synple is hosted in github at https://github.com/callendeprieto/synple
and can be obtained using {\tt git}
\\ {\tt git clone https://github.com/callendeprieto/synple synple} \\
\noindent or by downloading a zip file from the website.
Your Python (3.x) installation will require the packages {\tt subprocess}, {\tt numpy}, and {\tt scipy}, usually obtained with {\tt pip} (e.g. {\tt pip3 install numpy}). You probably want to install ipython and matplotlib as well, since we will be using that in the examples below.
The installation requires a FORTRAN compiler, and the GNU compiler is used by default
\\ {\tt cd synple/synspec ; make clean; make; cd ../..}.
The atomic and molecular line lists are sizable and need to be downloaded separately
\\ {\tt cd synple/linelists ; make clean; make; cd ../..} \\
\noindent where the automated download requires that {\tt wget} is available in your system, otherwise download the line lists manually from \\ {\tt ftp://carlos:allende@ftp.ll.iac.es/linelists} and copy them to the synple/linelists directory. For speed the linelists are converted to binary format by the same (make) script.
You can (optionally) download the Kurucz (2005) solar spectral atlas, which can be used for comparing the calculations done with Synple against real observations
\\ {\tt cd synple/atlases ; make clean; make; cd ../..}.
You need to make synple visible to Python by including the synple directory in your PYTHONPATH variable. Say you've placed the synple parent directory in your home, then you can add it in the linux shell by typing (or including in your .bashrc or .cshrc files)
\begin{table}[h]
\begin{tabular}{ll}
bash: & export PYTHONPATH="\$PYTHONPATH:\$HOME/synple" \\
csh: & setenv PYTHONPATH = "\$PYTHONPATH:\$HOME/synple" .
\end{tabular}
\end{table}
\section{Examples}
Once synple is installed, all you need is a model atmosphere to being using it. In this section we'll include a set of simple practical examples, mainly based on the three model atmospheres included in the synple/models directory: one is a solar Kurucz model ('ksun.mod'; Kurucz 1979 and later updates), one is a solar MARCS model ('msun.mod'; Gustafsson et al. 2008), and the third is a Phoenix model for Vega-like A-type star ('lte09600-4.00-0.0.PHOENIX-ACES-AGSS-COND-2011.ATMOS.fits') from Husser et al. (2013).
\subsection{Computing your first solar spectrum}
\label{6162}
\begin{figure}[t!]
\centering
\includegraphics[width=14cm]{Figure_1.ps}
\caption{Here's your first spectrum with synple. You have modeled the solar spectrum in the vicinity of the Ca I $\lambda$6162 line. The Ca I line is the strong line at the center, visibly damped by collisions with hydrogen atoms.
\label{first}
}
\end{figure}
For this exercise we'll use the Kurucz solar model included with synple. We're going to compute a piece of the spectrum around the Ca I $\lambda$6162 line. We start ipython and import the standard synthesis routine {\tt syn} from synple
\\
\\
\noindent {\tt
\$ ipython \\
Python 3.6.8 (default, Jan 14 2019, 11:02:34) \\
Type 'copyright', 'credits' or 'license' for more information \\
IPython 7.4.0 -- An enhanced Interactive Python. Type '?' for help. \\
\\
In [1]: from synple import syn \\
}
\noindent then request the computation of the spectrum from the model atmosphere in the file {\it ksun.mod} between 6160 and 6164 \AA\
\\
\\
\noindent {\tt
In [2]: wave, flux, cont = syn('ksun.mod', (6160,6164) ) \\
teff,logg,vmicro= 5777.0 4.437 2.0 \\
syn ellapsed time 48.8003294467926 seconds \\
}
\noindent We've got it! The routine {\tt syn} returns three numpy arrays with the wavelengths (wave), the fluxes (flux; $H_{\lambda}$), and the continuum flux (cont). If we wish to visualize the continuum-normalized spectrum, we can use matplotlib
\\
\\
\noindent {\tt
In [3]: pylab \\
Using matplotlib backend: TkAgg \\
Populating the interactive namespace from numpy and matplotlib \\
\\
In [4]: plot(wave,flux/cont) \\
}
\noindent and that's it! You should be looking at your first computed spectrum and it should look like the one in Fig. \ref{first}. In addition to the run with height of the thermodyanical quantities, the model atmosphere contains a detailed description of the chemical abundances and the micro-turbulence velocity (see below). These parameters are simply adopted from the model atmosphere, but can be changed if needed, as described in the next section.
\subsection{Altering micro-turbulence and chemical composition}
\label{abundances}
\begin{figure}[t!]
\centering
\includegraphics[width=7cm]{Figure_2a.ps}
\includegraphics[width=7cm]{Figure_2b.ps}
\caption{Repeating the calculation in Fig \ref{6162} (blue) but adding a second curve (orange) on the left panel reducing the micro-turbulence from 2 to 1 km s$^{-1}$, and on the right-hand panel increasen the Ca abundance by 0.2 dex.
\label{micro-abu}
}
\end{figure}
The model atmospheres we deal with are in hydrostatic equilibrium, and therefore pressure and gravity are in balance, so everything is at rest. This is unrealistic. Real stellar atmospheres have turbulence, shocks, convection, meridional circulation, etc. Thus, the computed line profiles are narrower than observed. One of the patches to address this problem is the so-called micro-turbulence velocity, which accounts for small-scale velocities of the absorbing particles. This includes small scale turbulence, and needs to be included in the computation of the linel absorption profile at the microscopic level, before solving the radiative transfer equation.
Synple includes micro-turbulence in the spectrum calculations automatically, if that's indicated in the model atmosphere file, but that value can be overridden by explicitly indicating it when calling the synthesis routine {\tt syn} using the parameter {\it vmicro}.
Let's repeat the example in \S \ref{6162} changing the micro-turbulence from the value used to construct the solar Kurucz model we used, 2 km s$^{-1}$, to a more reasonable value for a solar-like star of 1 km s$^{-1}$
\\
\\
\noindent {\tt
In [5]: wave2, flux2, cont2 = syn('ksun.mod', (6160,6164), vmicro = 1. ) \\
teff,logg,vmicro= 5777.0 4.437 1.0 \\
}
\noindent which can be easily compared with the previous calculation
\\
\\
\noindent {\tt
In [6]: plot(wave2,flux2/cont2) \\
}
\noindent as illustrated in the left-hand panel of Fig. \ref{micro-abu}. The weak, unsaturated, lines, and the core of the strong Ca I $\lambda$6162 line, are less broadened (brown curve) after reducing the micro-turbulence, while the damping wings of strong lines are insensitive to this parameter.
Similarly to the micro-turbulence, the chemical abundances can be changed from those used in the construction of the model atmosphere when computing the detailed spectrum. Since the most direct effect of the change of the abundance of an element (other than hydrogen) in the atmosphere is on the strength of its spectral lines, this is usually a good approximation for most elements and for reasonably small changes in abundances. But many elements, especially the most abundant ones, affect the thermodynamics of the atmosphere, and therefore for those elements this is a risky approximation to make. On the other hand, the approximation is very good for trace elements.
To supersede the abundances in the model atmosphere we can call {\tt syn} with the keyword {\it abu}. The abundances are expressed as the number density of nucleii of the elements relative to that of hydrogen
\begin{equation}
\epsilon (X) = \frac{N(X)}{N(H)}.
\end{equation}
Let's read the ones in the model atmosphere and then increase the calcium abundance by 50\% (0.2 dex)
\\
\\
\noindent {\tt
In [7]: from synple import read\_model \\
In [8]: atmostype, teff, logg, vmicro, abu, nd, atmos = read\_model('ksun.mod') \\
In [9]: abu[19] = abu[19] * 1.5 \\
In [10]: wave3, flux3, cont3 = syn('ksun.mod', (6160,6164), vmicro = 1. , abu=abu ) \\
teff,logg,vmicro= 5777.0 4.437 1.0. \\
In [11]: clf() \\
In [12]: plot(wave2,flux2/cont2, wave3, flux3/cont3).
}
\\
\\
This calculation is shown in the right-hand panel of Fig. \ref{micro-abu}, and it reveals that there are three Ca I lines in the computed spectral segment.
\subsection{Additional line broadening}
\label{fwhm}
\begin{figure}[t!]
\centering
\includegraphics[width=14cm]{Figure_3.ps}
\caption{Repeating the calculation in Fig \ref{6162} (blue) but adding the result of a convolution with a rotational profile for $v \sin i = 5$ km s$^{-1}$ (orange), a Gaussian kernel with a FWHM of 0.2 \AA\ (green), and both (brown).
\label{convolution}
}
\end{figure}
The spectral lines in a computed spectrum are naturally broadened due to the uncertainty principle, micro-turbulence (see Section \ref{abundances}), the thermal velocities of the absorbing atoms and molecules, and the collisions they suffer with surrounding free electrons and hydrogen atoms. All these broadening factors are included in the calculations done as described in the previous exercise, but there are additional sources of uncertainty that may be significant for your particular application.
\begin{itemize}
\item \underline{macro-turbulence}: while the {\it micro} takes care of small-scale velocity fields by introducing broadening at the microscopic level, broadening the line profiles at each atmospheric layer, there are velocities on scales much larger than the photon mean free-path that need to be taken into account by convolution of the computed spectrum. This is usually taken into account by convolving with a Gaussian velocity kernel, or with a radian-tangencial profile (see Gray xxxx). Synple implements convolution with a Gaussian velocity field in the routine {\tt vgconv}.
\item \underline{rotation}: stellar rotation broadens the spectral profiles. To be exact this has to be taken into account numerically, by Doppler-shifting the intensity contributions from different angles ($\theta$) in Eq. \ref{flux}. Nevertheless the effect or rotation can be well approximated by a covolution of the flux computed for no rotation with a particular kernel (see Gray xxxx). This is implemented in Synple in the routine {\tt rotconv}.
\item \underline{instrumental profile}: Instruments distort the stellar spectrum by convolving it with the instrumental profile. If the resolving power is constant, this can be usually approximated as a macro-turbulence, with a Gaussian kernel with a constant width in velocity space. Sometimes is the resolution, the FWHM in wavelength of the response of the instrument to a monochromatic source, what is constant, and the instrumental profile can be handle in Synple with the routine {\tt lgconv}.
\end{itemize}
\begin{figure}[t!]
\centering
\includegraphics[width=14cm]{Figure_4.ps}
\caption{In addition to the original calculation in Fig. \ref{6162} (blue line), we show the result of the convolution with a rotational profile for $v \sin i = 5$ km s$^{-1}$ and a Gaussian kernel with a FWHM of 0.2 \AA\ using {\tt rotconv}{\tt lgconv} (green) and rotin (orange).
\label{rotin}
}
\end{figure}
The following example demonstrates how to convolve with a rotational profile ($vsini = 5. $ km s$^{-1}$), a Gaussian profile with a constant resolution FWHM = 0.2 \AA\, and both, the original calculation in \S \ref{6162}
\\
\\
\noindent {\tt
In [13]: from synple import rotconv, lgconv \\
In [14]: wave2, flux2 = rotconv(wave, flux/cont, 5.) \\
In [15]: wave3, flux3 = lgconv(wave, flux/cont, 0.2) \\
In [16]: wave4, flux4 = lgconv(wave2, flux2, 0.2) \\
In [17]: clf() \\
In [18]: plot(wave, flux/cont, wave2,flux2, wave3, flux3, wave4, flux4).
}
\\
\\
\noindent Note that the spectral range of the output spectrum is truncated in wavelength, since it is computed only for the frequencies with information in the original calculation.
These routines for convolution are directly implemented in Python. Synspec has a companion FORTRAN program that handles the convolution with the instrumental or rotational profiles: rotin. One can use this program by including the {\it fwhm} and {\it vrot} parameters when calling {\tt syn} as in the following example
\noindent {\tt
In [19]: wave2, flux2, cont2 = syn('ksun.mod', (6160,6164) , vrot = 5.0, fwhm = 0.2 ) \\
In [20]: clf() \\
In [21]: plot(wave, flux/cont, wave2, flux2/cont2, wave4, flux4)
}
\\
\noindent Note the different behaviour for rotin (orange curve in Fig. \ref{rotin}), which does not trim the edges of the computed spectrum, and {\tt lgconv}/{\tt rotconv} (green). Rotin does not include convolution with a Gaussian kernel with a constant width in velocity, implemented in {\tt vgconv}.
\subsection{Multiple models}
One often faces the need to compute the spectra for multiple models. Since the sampling of frequencies is internally controlled within synspec, it becomes desirable to force the output fluxes to be on the same wavelength grid, and this can be done using the parameter {\it dw} in the routine {\tt syn}.
When using synple, the default value for the variable {\tt modeldir} points to the folder {\tt models} inside you {\tt synple} parent directory. If the model atmospheres are in your working directory, or as in the first examples below, the models are in the {\tt models} folder, that's ok, but if you want to use models elsewhere you will need to change {\tt modeldir} to point to the right path (changing the source code in synple.py) or simply passing the complete filenames, including an absolute path.
\begin{figure}[t!]
\centering
\includegraphics[width=14cm]{Figure_5.ps}
\caption{We now use all the models in the 'modeldir' directory in one command, with multiple values of the micro, using {\tt multisyn}.
\label{rotin}
}
\end{figure}
If you have a bunch of models you want to compute spectra for, or multiple values of vrot, fwhm, or vmicro, you can wrap around the routine syn, or you can use the macro {\tt multisyn}, after setting the file names in a list like in this example
\noindent {\tt
In [22]: from synple import multisyn \\
In [23]: import glob \\
In [24]: import os.path \\
In [25]: modeldir = "/home/callende/synple/models" \\
In [26]: models = glob.glob(os.path.join(modeldir,"*mod")) \#get the models in a list \\
In [27]: wave5, flux5, cont5 = multisyn(models, (6160,6164), vmicro = [1.,2.,4.] ) \\
In [28]: clf() \\
In [29]: for i in range(len(models)): plot(wave5, flux5[i,:]/cont5[i,:])\\
\\
}
\\
\noindent and the wavelength array will now be common to all spectra, and the flux and cont arrays returned will be two-dimensional, with the first dimention running along the models in the input list.
\section{Identification of spectral features}
\label{tag}
Synple can be used to identify which transitions are causing any given spectral feature. Of course, to succeed you need to use a line list including the relevant transitions, with data of sufficient accuracy.
As we have seen, the usual output from the routine {\tt syn} is a tuple with three arrays: wavelengths, fluxes and continuum fluxes. When the parameter {\tt tag} is set to {\bf True} in {\tt syn}, the output changes including a 4-th element, a list with three additional arrays that give
\begin{enumerate}
\item the wavelengths of the most relevant transitions,
\item the ions or molecules responsible for those transitions, and
\item the estimated equivalent widths associated with them (in milliangstroms).
\end{enumerate}
\begin{figure}[t!]
\centering
\includegraphics[width=14cm]{Figure_6.ps}
\caption{The main transitions in the spectrum can be labeled activating the {\tt tag} keyword in {\tt syn}.
\label{tagging}
}
\end{figure}
For example, for the very first spectrum computed in section \ref{6162}, we could have used this feature
\noindent {\tt \\
In [1]: from synple import syn, tags\\
\\
In [2]: d = syn('ksun.mod', (6160,6164) , tag = True)\\
}
\\
\noindent to produce the output graphics shown in Figure \ref{tagging}. The routine {\tt tags} can be used to plot the output from syn for transitions expected to be stronger than an specified threshold in equivalent width, e.g.
\noindent {\tt \\
In [3]: tags(d, 1.)
}
\\
\noindent will tag several several additional features estimated to produce absorptions stronger than 1
m\AA, and not included when the default minimum of 10 m\AA\ is used.
\section{Grid handling}
Synple includes a number of tools for creating grids of synthetic spectra. The format adopted is the same used for the FERRE grids, described in Section 4 of the FERRE manual available from
{\tt https://github.com/callendeprieto/ferre/blob/master/docs/ferre.pdf}
\\
Here is a quick overview of the various tools.
\begin{itemize}
\item head\_synth(synthfile): extracts the header of a grid
\item lambda\_synth(synthfile): extracts the wavelength array
\item read\_synth(synthfile,nd=False): reads the header, parameters and fluxes from a file
\item write\_synth(synthfile,d,hdr=None): writes a grid to file
\item fill\_synth(d,kernel='thin\_plate\_spline',neighbors=100): fills-in missing data using Radial Basis Functions (RBF) interpolation
\item rbf\_get(synthfile, kernel='thin\_plate\_spline'): finds the coefficients for RBF interpolation
\item rbf\_apply(synthfile,c,par): applies the RBF coefficients to interpolate
\item gsynth(synthfile,...): applies smoothing and reddening to an existing grid
\item polysyn(modelfiles, wrange, ...): sets up a directory tree for computing spectra for a grid using a job scheduler such as slurm
\item collect\_marcs(modeldir=modeldir, tteff=None, ...): collects MARCS model atmospheres for grid computation
\item collect\_kurucz(modeldir=modeldir, tteff=None, ...): collects Kurucz model atmospheres for grid computation
\item collect\_k2odfnew(modeldir=modeldir, ...): collects Kurucz ODFNEW model atmospheres for grid computation
\item mkgrid(synthfile=None, tteff=None, ...): collects the results from a calculation prepared using polysyn for a regular grid and stores the spectra in FERRE format
\item mkgrid\_irregular(synthfile=None, tteff=None, ...): collects the results from a calculation prepared using polysyn for an irregular grid and stores the spectra in FERRE format.
\end{itemize}
\section{Computing opacity tables}
\begin{figure}[t!]
\centering
\includegraphics[width=14cm]{Figure_7.ps}
\caption{Opacity in the range 6100--6110. \AA\ for four combinations of a pair of densities ($\log_{10} \rho = -32.236191, -29.933606$) and temperatures ($\log_{10} T = 8.059055, 8.51957$) and solar abundances.
\label{opacity-fig}
}
\end{figure}
Synple provides simplified access to the most basic features for opacity table calculations available with synspec. The main subroutines are
\begin{itemize}
\item polyopt(wrange=(9.e2,1.e5), dlw=2.1e-5, ...): sets up an opacity grid calculation
\item read\_opt(filename): reads an opacity table
\item read\_copt(filename,nrho,nt): reads the continuum opacities from an opacity grid calculation.
\end{itemize}
For example, to compute a minimalist table covering 10 \AA\ (6100. -6110. \AA), 2 temperatures (3163 and 5012 K), and 2 densities (1e-14, 1e-13 gr cm$^{-3}$):
\noindent {\tt
In [1]: from synple import polyopt \\
In [2]: polyopt(wrange=(6100.,6110.),tlt=(2,3.5,0.2),tlrho=(2,-14.,1.0)) \\
}
\\
The code creates 1 folder named {\tt hyd0000001} (you would get more folders by
including more chemical mixtures, but the default is to assume solar abundances)
with a script {\it hyd0000001.job}. Executing the script should produce an output text file {\bf opt.data} with the opacity table.
To read and plot the table
\noindent {\tt
In [1]: from synple import read\_opt \\
In [2]: import matplotlib.pyplot as plt \\
In [3]: lrho,lt,lambda0,lopa,abu\_eos,abu\_opa = read\_opt('opt.data')\\
In [4]: plt.plot(lambda0,lopa[:,0,0]) \\
In [5]: plt.plot(lambda0,lopa[:,0,1]) \\
In [6]: plt.plot(lambda0,lopa[:,1,0]) \\
In [7]: plt.plot(lambda0,lopa[:,1,1]) \\
In [8]: plt.xlabel('wavelength (A)') \\
In [9]: plt.ylabel('log10 specific opacity (cm2/gr)') \\
In [10]: plt.show().
}
\\
\noindent which will produce the output shown in Figure \ref{opacity-fig}.
\begin{figure}[t!]
\centering
\includegraphics[width=14cm]{Figure_8.ps}
\caption{Example of the computation of emergent specific intensities I$_{\lambda}$ for various directions ($\mu = \cos \theta = 1$ the highest and $\mu = \cos \theta = 0.0001$ the lowest). The units are in erg cm$^{-2}$ s$^{-1}$ \AA$^{-1}$ steradian$^{-1}$.
\label{intensity-fig}
}
\end{figure}
\section{Computing emergent intensities $I_{\lambda}$}
It is very easy to tweak the basic routine {\it syn} (see Sect. \ref{6162}),
or the parallel versions {\it polysyn} or {\it raysyn}, to output the
specific intensity as a function of the angle from the vertical ($\theta$).
One simply needs to set the keyword {\tt intensity} to true, as in the
following example. When this is activated the output from {\tt syn} will
change from a tuple with 3 arrays (4 if {\tt tag} is set,
as explained in Sect. \ref{tag}) to a tuple with 5 arrays
(6 if {\tt tag} is set), and
the 4th array will be a 2D matrix with the emergent intensity for
10 inclinations corresponding to
$\mu \equiv = \cos \theta = 0.0001, 0.001, 0.01, 0.1, 0.25, 0.4, 0.55, 0.7, 0.85, and 1.0$, while the 5th array will correspond to the continuum intensity
for the same angles.
\\
\\
\noindent {\tt
In [1]: from synple import syn
\\
In [2]: import matplotlib.pyplot as plt
\\
In [3]: wave, flux, con, inte, coninte = syn('ksun.mod', (6160,6164), intensity=True ) \\
/home/callende/synple/models/ksun.mod is a kurucz model
\\
teff,logg,vmicro= 5777.0 4.437 2.0 \\
syn ellapsed time 16.27164101600647 seconds \\
\\
In [4]: for angle in range(10): plt.plot(wave,inte[:,angle])
\\
In [5]: plt.ylabel('\$I\_\{$\backslash$lambda\}\$ (erg/s/cm2/A/steradian)')
\\
In [6]: plt.xlabel('Wavelength (angstroms)')
\\
In [7]: plt.show()
\\
}
\noindent which will produce the graph shown in Fig. \ref{intensity-fig}. Note that this option is not compatible with the broadening parameters {\tt fwhm}, {\tt vrot} or {\tt vmacro}.
\section{References}
\begin{itemize}
\item Allende Prieto, C., Fern{\'a}ndez-Alvar, E., Schlesinger, K.~J., et al.\ 2014, A\&A, 568, A7
\item Gustafsson, B., Edvardsson, B., Eriksson, K., et al.\ 2008, A\&A, 486, 951
\item Hubeny, I. \& Lanz, T.\ 2017, arXiv:1706.01859
\item Hubeny, I., Allende Prieto, C., Osorio, Y., et al.\ 2021, arXiv:2104.02829
\item Husser, T.-O., Wende-von Berg, S., Dreizler, S., et al.\ 2013, A\&A, 553, A6
\item Kurucz, R.~L.\ 1979, ApJS, 40, 1
\end{itemize}
\end{document}
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\contentsline {section}{\numberline {1}Introduction}{2}{}%
\contentsline {section}{\numberline {2}Installing}{2}{}%
\contentsline {section}{\numberline {3}Examples}{3}{}%
\contentsline {subsection}{\numberline {3.1}Computing your first solar spectrum}{3}{}%
\contentsline {subsection}{\numberline {3.2}Altering micro-turbulence and chemical composition}{4}{}%
\contentsline {subsection}{\numberline {3.3}Additional line broadening}{5}{}%
\contentsline {subsection}{\numberline {3.4}Multiple models}{7}{}%
\contentsline {section}{\numberline {4}Identification of spectral features}{8}{}%
\contentsline {section}{\numberline {5}Grid handling}{9}{}%
\contentsline {section}{\numberline {6}Computing opacity tables}{9}{}%
\contentsline {section}{\numberline {7}Computing emergent intensities $I_{\lambda }$}{10}{}%
\contentsline {section}{\numberline {8}References}{11}{}%
+28
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#
# makefile for downloading synple/bas/FERRE grids
# Carlos 2024
#
FTP = ftp://carlos:allende@ftp.ll.iac.es/grids/
WGET = `which wget`
#general line lists
STANDARD = n_sc2-BRZ-DESIrbf.pickle n_sc2-LAMOSTrbf.pickle n_sc2-STISrbf.pickle n_sc2-XPrbf.pickle n_sc2-STIS-NICMOSrbf.pickle n_sc2-OSIRIS-R2500Urbf.pickle n_sc2-IDS-R900Vrbf.pickle n_DA-STISrbf.pickle
all:
$(call sequence, $(STANDARD))
clean:
rm -f *.pickle
define sequence
for file in $(1) ; do \
${WGET} ${FTP}$$file ; \
done
endef
+33
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35000. 4.0 ! TEFF, GRAV
F F ! LTE, LTGRAY
'' ! no change of general optional parameters
*-----------------------------------------------------------------
* frequencies
50 ! NFREAD
*-----------------------------------------------------------------
* data for atoms
*
8 ! NATOMS
* mode abn modpf
2 0 0
2 0 0
0 0 0
0 0 0
0 0 0
1 0 0
1 0 0
1 0 0
*-----------------------------------------------------------------
* data for ions
*
*iat iz nlevs ilast ilvlin nonstd typion filei
*
1 0 9 0 0 0 ' H 1' './data/h1.dat'
1 1 1 1 0 0 ' H 2' ' '
2 0 14 0 0 0 'He 1' './data/he1.dat'
2 1 14 0 0 0 'He 2' './data/he2.dat'
2 2 1 1 0 0 'He 3' ' '
0 0 0 -1 0 0 ' ' ' '
*
* end
+377
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1*******************************
M O D E L A T M O S P H E R E
*******************************
TEFF = 35000.
LOG G = 4.00
INPUT KEYWORD PARAMETERS:
-------------------------
CHEMICAL ELEMENTS INCLUDED
--------------------------
NUMBER ELEMENT ABUNDANCE
A=N(ELEM)/N(H) A/A(SOLAR)
1 H 1.00E+00 1.00E+00 EXPLICIT: IAT= 1
2 He 8.51E-02 1.00E+00 EXPLICIT: IAT= 2
6 C 2.45E-04 1.00E+00
7 N 6.03E-05 1.00E+00
8 O 4.57E-04 1.00E+00
YTOT WMY WMM 1.08588 1.35982D+00 2.09547D-24
0
EXPLICIT IONS INCLUDED
----------------------
NO. ION N0 N1 NK IZ IUPSUM ICUP FF
1 H 1 1 9 10 1 -100 16 0.000D+00
2 He 1 11 24 25 1 0 16 0.000D+00
3 He 2 25 38 39 2 0 32 0.000D+00
iopadd,irsct,irsche,irsch2,iophmi,ioph2p,iopoh,iopch 4 1 1 0 1 0 0 0
0
EXPLICIT ENERGY LEVELS INCLUDED
-------------------------------
NO. LEVEL ION ION.FREQ.(s^-1) G NQ IEL ILK IAT IMOD ILT IIE IIF
1 (N=1) H 1 3.2880500D+15 2.00 1 1 0 1 7 0 -1 1
2 (N=2) H 1 8.2201250D+14 8.00 2 1 0 1 7 0 -2 2
3 (N=3) H 1 3.6533889D+14 18.00 3 1 0 1 7 0 -3 3
4 (N=4) H 1 2.0550313D+14 32.00 4 1 0 1 7 0 -4 4
5 (N=5) H 1 1.3152200D+14 50.00 5 1 0 1 7 0 -5 5
6 (N=6) H 1 9.1334722D+13 72.00 6 1 0 1 7 0 -5 6
7 (N=7) H 1 6.7103061D+13 98.00 7 1 0 1 7 0 -5 7
8 (N=8) H 1 5.1375781D+13 128.00 8 1 0 1 7 0 -5 8
9 (N=9) H 1 0.0000000D+00 162.00 9 1 0 1 7 0 -5 9
10 H 2 H 1 0.0000000D+00 1.00 1 1 1 1 7 0 -6 10
11 1 sing S He 1 5.9450352D+15 1.00 1 2 0 2 7 0 -7 11
12 2 trip S He 1 1.1526721D+15 3.00 2 2 0 2 7 0 -8 12
13 2 sing S He 1 9.6014543D+14 1.00 2 2 0 2 7 0 -9 13
14 2 trip P He 1 8.7593372D+14 9.00 2 2 0 2 7 0 -10 14
15 2 sing P He 1 8.1453622D+14 3.00 2 2 0 2 7 0 -11 15
16 3 trip S He 1 4.5172735D+14 3.00 3 2 0 2 7 0 -12 16
17 3 sing S He 1 4.0292112D+14 1.00 3 2 0 2 7 0 -12 17
18 3 trip P He 1 3.8193564D+14 9.00 3 2 0 2 7 0 -12 18
19 3 trip D He 1 3.6583679D+14 15.00 3 2 0 2 7 0 -12 19
20 3 sing D He 1 3.6574687D+14 5.00 3 2 0 2 7 0 -12 20
21 3 sing P He 1 3.6259902D+14 3.00 3 2 0 2 7 0 -12 21
22 4 trip S He 1 2.4004386D+14 3.00 4 2 0 2 7 0 -13 22
23 4 sing S He 1 2.2079719D+14 1.00 4 2 0 2 7 0 -13 23
24 4 trip P He 1 2.1249294D+14 9.00 4 2 0 2 7 0 -13 24
25 (N=1) He 2 1.3157598D+16 2.00 1 3 2 2 7 0 -14 25
26 (N=2) He 2 3.2893994D+15 8.00 2 3 0 2 7 0 -15 26
27 (N=3) He 2 1.4619553D+15 18.00 3 3 0 2 7 0 -16 27
28 (N=4) He 2 8.2234986D+14 32.00 4 3 0 2 7 0 -17 28
29 (N=5) He 2 5.2630391D+14 50.00 5 3 0 2 7 0 -18 29
30 (N=6) He 2 3.6548882D+14 72.00 6 3 0 2 7 0 -18 30
31 (N=7) He 2 2.6852240D+14 98.00 7 3 0 2 7 0 -18 31
32 (N=8) He 2 2.0558746D+14 128.00 8 3 0 2 7 0 -18 32
33 (N=9) He 2 1.6243948D+14 162.00 9 3 0 2 7 0 -18 33
34 (N=10) He 2 1.3157598D+14 200.00 10 3 0 2 7 0 -18 34
35 (N=11) He 2 1.0874048D+14 242.00 11 3 0 2 7 0 -18 35
36 (N=12) He 2 9.1372206D+13 288.00 12 3 0 2 7 0 -18 36
37 (N=13) He 2 7.7855608D+13 338.00 13 3 0 2 7 0 -18 37
38 (N=14) He 2 6.7130600D+13 392.00 14 3 0 2 7 0 -18 38
39 He 3 He 2 0.0000000D+00 1.00 1 3 3 2 7 0 -19 39
ils,ijfl 25 21 13289173674059048.
MAXIMUM NUMBER OF OVERLAPPING TRANSITIONS: 7
ACCURACY OF INTEGRATIONS:
Interval: 2.80000000E+16 1.00000000E+12 2.79990000E+16 2.79990003E+16
Planck functions: 17500. 2.3673E-04
35000. 4.0044E-04
70000. 1.0039E-04
TOTAL NUMBER OF FREQUENCIES: 3146
SELECTED FREQUENCIES: 3133
0
FREQUENCY POINTS AND WEIGHTS - EXPLICIT
---------------------------------------
IJ FREQ WEIGHT PROF
19 1.40247150D+16 2.45180439D+14 0.00000D+00
20 1.36569443D+16 4.90360892D+14 0.00000D+00
21 1.32891737D+16 1.64259068D+14 0.00000D+00
32 5.29702636D+15 1.70995639D+14 0.00000D+00
33 4.76732373D+15 3.84350582D+14 0.00000D+00
34 4.29059136D+15 4.52895754D+14 0.00000D+00
35 3.86153222D+15 4.07606179D+14 0.00000D+00
36 3.47537900D+15 2.69619403D+14 0.00000D+00
37 3.32229341D+15 9.09297079D+13 0.00000D+00
154 2.46604814D+15 1.06376566D+10 3.15594D-14
155 2.46603750D+15 1.06376566D+10 3.16517D-14
156 2.46602686D+15 1.06376566D+10 3.15594D-14
204 2.92271111D+15 2.51750618D+10 5.07557D-15
249 3.08254688D+15 2.65518230D+10 1.76373D-15
452 4.56673612D+14 3.02381655D+10 2.41083D-13
485 6.16509376D+14 4.08210986D+10 1.63870D-14
EXTERNAL IRRADIATION - EXTOT0, EXTOT: 0.000E+00 0.000E+00
VALUES OF SOME KEYWORD PARAMETERS:
==================================
ISPLIN= 0 IRTE = 0 IBC = 3 ILMCOR= 3 ILPSCT= 1
ILASCT= 0 DJMAX = 0.001 NTRALI= 3 IPSLTE= 0
ICOMPT= 0
IZSCAL= 0 IBCHE = 1 IVISC = 0
IFALI = 5 IFPOPR= 4 JALI = 1 IFRALI= 0
IFPREC= 1 IELCOR= -1 ICHC = 1 IRSPLT= 1 IATREF= 1
MODREF= 1 IACPP = 7 IACPD = 0 IFLEV = 0 IDLTE = 1000
POPZER=1.E-20 POPZR2=1.E-20 RADZER=1.E-20 NITZER= 1 IFDIEL= 0
IOVER = 1 ITLAS = 100
NITER = 30 NLAMBD= 2 ND = 70
JIDS = 0 IDMFIX= 1
NMU = 3
NELSC = 0 IHECOR= 0 IBFINT= 1 IRDER = 3 CHMAX = 0.001
ILDER = 0 IBPOPE= 1 CHMAXT= 0.010 NLAMT = 1
INTRPL= 0 ICHANG= 0
INHE = 1 INRE = 2 INPC = 3 INSE = 4 INMP = 0
INDL = 0 NDRE = 0 TAUDIV= 0.500 IDLST = 5 NRETC = 0
ICONV = 0 IPRESS= 0 ITEMP = 0
IOPADD= 4 IRSCT = 1 IOPHMI= 1 IOPH2P= 0
IACC = 7 IACD = 4 KSNG = 0 ITEK = 4 ORELAX= 1.000
IWINBL= -1
ICRSW = 0 SWPFAC= 0.100 SWPLIM= 0.001 SWPINC= 3.000
IFPRD = 0 XPDIV = 3.0
TRAD = 0. WDIL =0.000
HMIX0 = -1.0 VTB = 0. 1
XGRAD = 0.00 STRL1 =1.E-03 STRL2 =2.E-02
STRLX =1.E-10
FRCMAX=0.E+00 FRCMIN=1.E+12 FRLMAX=2.E+16 FRLMIN=1.E+13
CFRMAX= 2.00
DFTAIL= 0.250 NFTAIL= 21
TSNU = 0. VTNU = 0.00 DDNU = 0.750
IELNU = 0 CNU1 = 4.50 CNU2 = 3.00
ISPODF= 0
DPSILG= 10.00 DPSILT= 1.25 DPSILN= 10.00 DPSILD= 1.25
ICOMST= 1 ICOMDE= 1 ICOMBC= 1
ICMDRA= 0 KNISH = 0
NCFOR1= 0 NCFOR2= 1 NCCOUP= 0 NCITOT= 1 NCFULL= 1
Total number of lines : 137
Number of weak lines : 0
Intermediate lines : 8
Number of strong lines: 129
MAXIMUM NUMBER OF OVERLAPPING TRANSITIONS: 7
ACCURACY OF INTEGRATIONS:
Interval: 2.80000000E+16 1.00000000E+12 2.79990000E+16 2.79990003E+16
Planck functions: 17500. 2.3673E-04
35000. 4.0044E-04
70000. 1.0039E-04
TOTAL NUMBER OF FREQUENCIES: 3146
SELECTED FREQUENCIES: 3098
SCHEME OF RADIATIVE EQUIL. DETERMINED IN RESOLV
ONLY INTEGRAL EQUATION FOR ID <= 49
BOTH FOR 50 <= ID <= 65
SCHEME OF RADIATIVE EQUIL. DETERMINED IN RESOLV
ONLY INTEGRAL EQUATION FOR ID <= 49
BOTH FOR 50 <= ID <= 65
REFERENCE LEVEL INDICES AS FUNCTIONS OF DEPTH
ITER =
ID= 1 10 39
ID= 2 10 39
ID= 3 10 39
ID= 4 10 39
ID= 5 10 39
ID= 6 10 39
ID= 7 10 39
ID= 8 10 39
ID= 9 10 39
ID= 10 10 39
ID= 11 10 39
ID= 12 10 39
ID= 13 10 39
ID= 14 10 39
ID= 15 10 39
ID= 16 10 39
ID= 17 10 39
ID= 18 10 39
ID= 19 10 25
ID= 20 10 25
ID= 21 10 25
ID= 22 10 25
ID= 23 10 25
ID= 24 10 25
ID= 25 10 25
ID= 26 10 25
ID= 27 10 25
ID= 28 10 25
ID= 29 10 25
ID= 30 10 25
ID= 31 10 25
ID= 32 10 25
ID= 33 10 25
ID= 34 10 25
ID= 35 10 25
ID= 36 10 25
ID= 37 10 25
ID= 38 10 25
ID= 39 10 25
ID= 40 10 25
ID= 41 10 25
ID= 42 10 25
ID= 43 10 25
ID= 44 10 25
ID= 45 10 25
ID= 46 10 25
ID= 47 10 25
ID= 48 10 25
ID= 49 10 25
ID= 50 10 25
ID= 51 10 39
ID= 52 10 39
ID= 53 10 39
ID= 54 10 39
ID= 55 10 39
ID= 56 10 39
ID= 57 10 39
ID= 58 10 39
ID= 59 10 39
ID= 60 10 39
ID= 61 10 39
ID= 62 10 39
ID= 63 10 39
ID= 64 10 39
ID= 65 10 39
ID= 66 10 39
ID= 67 10 39
ID= 68 10 39
ID= 69 10 39
ID= 70 10 39
**** KANTOROVICH acceleration: ITER 5
**** KANTOROVICH acceleration: ITER 6
**** ACCEL2, ITER= 7
**** KANTOROVICH acceleration: ITER 8
**** KANTOROVICH acceleration: ITER 9
**** KANTOROVICH acceleration: ITER 10
**** ACCEL2, ITER= 11
**** KANTOROVICH acceleration: ITER 12
**** KANTOROVICH acceleration: ITER 13
**** KANTOROVICH acceleration: ITER 14
**** ACCEL2, ITER= 15
**** KANTOROVICH acceleration: ITER 16
**** KANTOROVICH acceleration: ITER 17
**** KANTOROVICH acceleration: ITER 18
**** ACCEL2, ITER= 19
**** KANTOROVICH acceleration: ITER 19
**** KANTOROVICH acceleration: ITER 20
**** KANTOROVICH acceleration: ITER 21
**** KANTOROVICH acceleration: ITER 22
**** ACCEL2, ITER= 23
**** KANTOROVICH acceleration: ITER 23
**** KANTOROVICH acceleration: ITER 24
**** KANTOROVICH acceleration: ITER 25
**** KANTOROVICH acceleration: ITER 26
**** ACCEL2, ITER= 27
**** KANTOROVICH acceleration: ITER 27
**** KANTOROVICH acceleration: ITER 28
************************************
FINAL RESULTS:
MODEL QUANTITIES IN 28. ITERATION
************************************
TOTAL SURFACE FLUX 6.77712339D+12
----------------------
FINAL MODEL ATMOSPHERE
----------------------
ID MASS TAUROSS TEMP NE DENS P_gas LOG(G_rad) RAD/TOT CON/TOT (RAD+CON)/TOT
1 2.917E-07 5.001E-08 32890.1 3.011E+08 5.840E-16 2.632E-03 2.989E+00 1.001E+00 0.000E+00 1.00106E+00
2 3.974E-07 8.627E-08 32896.2 4.101E+08 7.956E-16 3.587E-03 2.989E+00 1.001E+00 0.000E+00 1.00106E+00
3 5.433E-07 1.363E-07 32903.0 5.605E+08 1.087E-15 4.903E-03 2.989E+00 1.001E+00 0.000E+00 1.00106E+00
4 7.447E-07 2.053E-07 32910.0 7.680E+08 1.490E-15 6.721E-03 2.989E+00 1.001E+00 0.000E+00 1.00106E+00
5 1.035E-06 3.049E-07 32916.6 1.067E+09 2.071E-15 9.341E-03 2.989E+00 1.001E+00 0.000E+00 1.00106E+00
6 1.436E-06 4.423E-07 32921.1 1.480E+09 2.873E-15 1.296E-02 2.989E+00 1.001E+00 0.000E+00 1.00106E+00
7 1.989E-06 6.319E-07 32922.8 2.050E+09 3.981E-15 1.795E-02 2.989E+00 1.001E+00 0.000E+00 1.00106E+00
8 2.752E-06 8.931E-07 32919.9 2.835E+09 5.508E-15 2.483E-02 2.989E+00 1.001E+00 0.000E+00 1.00106E+00
9 3.803E-06 1.253E-06 32906.6 3.919E+09 7.619E-15 3.432E-02 2.989E+00 1.001E+00 0.000E+00 1.00106E+00
10 5.254E-06 1.750E-06 32876.3 5.417E+09 1.054E-14 4.741E-02 2.989E+00 1.001E+00 0.000E+00 1.00106E+00
11 7.254E-06 2.435E-06 32829.4 7.489E+09 1.458E-14 6.547E-02 2.989E+00 1.001E+00 0.000E+00 1.00106E+00
12 1.001E-05 3.379E-06 32774.7 1.035E+10 2.016E-14 9.037E-02 2.989E+00 1.001E+00 0.000E+00 1.00106E+00
13 1.382E-05 4.681E-06 32725.4 1.430E+10 2.787E-14 1.247E-01 2.989E+00 1.001E+00 0.000E+00 1.00106E+00
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2.348074E+05 3.868749E+05 1.289415E+05 7.719129E+04 7.073103E+04
2.325471E+04 2.080614E+05 6.116605E+11 2.137826E+09 1.305303E+09
1.469989E+09 1.859075E+09 2.385444E+09 3.025035E+09 3.763062E+09
4.577925E+09 5.423050E+09 6.190176E+09 6.645296E+09 6.409469E+09
5.243786E+09 3.932615E+14
7.267051E+04 7.324008E+15 1.421455E-08 8.483392E+09 6.657485E+09
1.107730E+10 1.769891E+10 2.619529E+10 3.602255E+10 4.512733E+10
4.684157E+10 5.746035E+10 6.246738E+15 9.506047E+05 1.204174E+05
3.534480E+04 3.009102E+05 9.631173E+04 7.579593E+04 2.446339E+04
2.171450E+05 3.580809E+05 1.193504E+05 7.146153E+04 6.590706E+04
2.169134E+04 1.941562E+05 4.843784E+11 2.864127E+09 1.927652E+09
2.246121E+09 2.885654E+09 3.733842E+09 4.756943E+09 5.929281E+09
7.205930E+09 8.482468E+09 9.511274E+09 9.789627E+09 8.702024E+09
6.335629E+09 5.267916E+14
7.857846E+04 9.742795E+15 1.890841E-08 1.133957E+10 1.005817E+10
1.711849E+10 2.755821E+10 4.086181E+10 5.588325E+10 6.804890E+10
6.410353E+10 6.138587E+10 8.309491E+15 6.858480E+05 1.102034E+05
3.265860E+04 2.791970E+05 8.963842E+04 7.182374E+04 2.323794E+04
2.064795E+05 3.407654E+05 1.135813E+05 6.801789E+04 6.311299E+04
2.079175E+04 1.861796E+05 3.967630E+11 3.829166E+09 2.821946E+09
3.394216E+09 4.424887E+09 5.769965E+09 7.381216E+09 9.212190E+09
1.116853E+10 1.301826E+10 1.421394E+10 1.377836E+10 1.104132E+10
7.109075E+09 7.009237E+14
8.500390E+04 1.283744E+16 2.491402E-08 1.503302E+10 1.494218E+10
2.597075E+10 4.209699E+10 6.248037E+10 8.473106E+10 9.904130E+10
8.218008E+10 6.256757E+10 1.094870E+16 5.131932E+05 1.028764E+05
3.075984E+04 2.639857E+05 8.499656E+04 6.925376E+04 2.245711E+04
1.997338E+05 3.298777E+05 1.099534E+05 6.585488E+04 6.145234E+04
2.026271E+04 1.815115E+05 3.335584E+11 5.076767E+09 4.070731E+09
5.042875E+09 6.664003E+09 8.751669E+09 1.123543E+10 1.402916E+10
1.693611E+10 1.945397E+10 2.044287E+10 1.828882E+10 1.301242E+10
7.469574E+09 9.236708E+14
9.198531E+04 1.672976E+16 3.246770E-08 1.969936E+10 2.176262E+10
3.856909E+10 6.290669E+10 9.336706E+10 1.250685E+11 1.380787E+11
9.824423E+10 6.130891E+10 1.426821E+16 3.953875E+05 9.732792E+04
2.934207E+04 2.527274E+05 8.158647E+04 6.751647E+04 2.193963E+04
1.953066E+05 3.227883E+05 1.075910E+05 6.444865E+04 6.045667E+04
1.995087E+04 1.787816E+05 2.863868E+11 6.652815E+09 5.768968E+09
7.345055E+09 9.828995E+09 1.299214E+10 1.672907E+10 2.087861E+10
2.503796E+10 2.816043E+10 2.806794E+10 2.272975E+10 1.430388E+10
7.453671E+09 1.203817E+15
9.957025E+04 2.157026E+16 4.186147E-08 2.551570E+10 3.109060E+10
5.610334E+10 9.201303E+10 1.364114E+11 1.795706E+11 1.835511E+11
1.099248E+11 5.830616E+10 1.839636E+16 3.127450E+05 9.313740E+04
2.829445E+04 2.445208E+05 7.913018E+04 6.643477E+04 2.163005E+04
1.927113E+05 3.187029E+05 1.062297E+05 6.364118E+04 5.999068E+04
1.981224E+04 1.775979E+05 2.506034E+11 8.617212E+09 8.035278E+09
1.049357E+10 1.420633E+10 1.888895E+10 2.437930E+10 3.037593E+10
3.607315E+10 3.939045E+10 3.661323E+10 2.644773E+10 1.483317E+10
7.165873E+09 1.552213E+15
1.078152E+05 2.757437E+16 5.351333E-08 3.278260E+10 4.374577E+10
8.026802E+10 1.322865E+11 1.956156E+11 2.513099E+11 2.323037E+11
1.162160E+11 5.428159E+10 2.351684E+16 2.545225E+05 9.044324E+04
2.767167E+04 2.398821E+05 7.780496E+04 6.620156E+04 2.159293E+04
1.925295E+05 3.185911E+05 1.061928E+05 6.362646E+04 6.024835E+04
1.991146E+04 1.785419E+05 2.238031E+11 1.107156E+10 1.104317E+10
1.476510E+10 2.020473E+10 2.700697E+10 3.491498E+10 4.336645E+10
5.078471E+10 5.324677E+10 4.531912E+10 2.898995E+10 1.471037E+10
6.715114E+09 1.984383E+15
1.167898E+05 3.508735E+16 6.809330E-08 4.207226E+10 6.108241E+10
1.138223E+11 1.883688E+11 2.773119E+11 3.443403E+11 2.802288E+11
1.174648E+11 4.979647E+10 2.992410E+16 2.146506E+05 8.986216E+04
2.767555E+04 2.406078E+05 7.820441E+04 6.737239E+04 2.201154E+04
1.964028E+05 3.251797E+05 1.083892E+05 6.494947E+04 6.175948E+04
2.042432E+04 1.831926E+05 2.049431E+11 1.420917E+10 1.508684E+10
2.061671E+10 2.849259E+10 3.826420E+10 4.951054E+10 6.117936E+10
7.023227E+10 6.968514E+10 5.332664E+10 3.022789E+10 1.412493E+10
6.185289E+09 2.525195E+15
1.265784E+05 4.466784E+16 8.668550E-08 5.443402E+10 8.547041E+10
1.615577E+11 2.682758E+11 3.921605E+11 4.641011E+11 3.229117E+11
1.147394E+11 4.522077E+10 3.809454E+16 1.895792E+05 9.242226E+04
2.863868E+04 2.496484E+05 8.130132E+04 7.085257E+04 2.318450E+04
2.070068E+05 3.429118E+05 1.143000E+05 6.849822E+04 6.538811E+04
2.163756E+04 1.941258E+05 1.937889E+11 1.838446E+10 2.068698E+10
2.884799E+10 4.023309E+10 5.425121E+10 7.018320E+10 8.603185E+10
9.598188E+10 8.842945E+10 5.985350E+10 3.028940E+10 1.325672E+10
5.631375E+09 3.214866E+15
1.372774E+05 5.717582E+16 1.109589E-07 7.165499E+10 1.210117E+11
2.317749E+11 3.858279E+11 5.578156E+11 6.164034E+11 3.560759E+11
1.092324E+11 4.077249E+10 4.876161E+16 1.772540E+05 9.956007E+04
3.102647E+04 2.711371E+05 8.845974E+04 7.792194E+04 2.553455E+04
2.281311E+05 3.780845E+05 1.260242E+05 7.553136E+04 7.236350E+04
2.395941E+04 2.150095E+05 1.905777E+11 2.420098E+10 2.874259E+10
4.084264E+10 5.743936E+10 7.771336E+10 1.003744E+11 1.215316E+11
1.300851E+11 1.086636E+11 6.429422E+10 2.942042E+10 1.224129E+10
5.085824E+09 4.115301E+15
1.373869E+05 5.731772E+16 1.112343E-07 7.185923E+10 1.214400E+11
2.326240E+11 3.872486E+11 5.597942E+11 6.180908E+11 3.563476E+11
1.091692E+11 4.073021E+10 4.888263E+16 1.772069E+05 9.966666E+04
3.106136E+04 2.714483E+05 8.856278E+04 7.802060E+04 2.556723E+04
2.284244E+05 3.785723E+05 1.261868E+05 7.562887E+04 7.245940E+04
2.399129E+04 2.152961E+05 1.905982E+11 2.426997E+10 2.883919E+10
4.098717E+10 5.764712E+10 7.799670E+10 1.007378E+11 1.219533E+11
1.304723E+11 1.088672E+11 6.432709E+10 2.940849E+10 1.223103E+10
5.080616E+09 4.125516E+15
+108
View File
@@ -0,0 +1,108 @@
16000. 2.0
F F ! LTE, LTGRAY
'BC16000g200v2.nst' ! name of file containing non-standard flags
*
* frequencies
*
2000
*
* atom for atoms
*
30 ! NATOMS
* mode abn modpf
2 0. 0 ! H
2 0. 0 ! He
0 0. 0
0 0. 0
0 0. 0
2 -2. 0 ! C
2 -2. 0 ! N
2 -2. 0 ! O
1 -2. 0
2 -2. 0 ! Ne
1 -2. 0
2 -2. 0 ! Mg
2 -2. 0 ! Al
2 -2. 0 ! Si
1 -2. 0
2 -2. 0 ! S
1 -2. 0
1 -2. 0
1 -2. 0
1 -2. 0
1 -2. 0
1 -2. 0
1 -2. 0
1 -2. 0
1 -2. 0
2 -2. 0 ! Fe
1 -2. 0
1 -2. 0
1 -2. 0
1 -2. 0
*
* atom for ions
*
*iat iz nlevs ilast ilvlin nonstd typion filei
*
1 0 9 0 0 0 ' H 1' 'atom/h1.dat'
1 1 1 1 0 0 ' H 2' ' '
2 0 24 0 0 0 'He 1' 'atom/he1.dat'
2 1 20 0 0 0 'He 2' 'atom/he2.dat'
2 2 1 1 0 0 'He 3' ' '
6 0 40 0 0 0 ' C 1' 'atom/c1_28+12lev.dat'
6 1 22 0 0 0 ' C 2' 'atom/c2_17+5lev.dat'
6 2 46 0 0 0 ' C 3' 'atom/c3_34+12lev.dat'
6 3 25 0 0 0 ' C 4' 'atom/c4_21+4lev.dat'
6 4 1 1 0 0 ' C 5' ' '
7 0 34 0 0 0 ' N 1' 'atom/n1_27+7lev.dat'
7 1 42 0 0 0 ' N 2' 'atom/n2_32+10lev.dat'
7 2 32 0 0 0 ' N 3' 'atom/n3_25+7lev.dat'
7 3 48 0 0 0 ' N 4' 'atom/n4_34+14lev.dat'
7 4 16 0 0 0 ' N 5' 'atom/n5_10+6lev.dat'
7 5 1 1 0 0 ' N 6' ' '
8 0 33 0 0 0 ' O 1' 'atom/o1_23+10lev.dat'
8 1 48 0 0 0 ' O 2' 'atom/o2_36+12lev.dat'
8 2 41 0 0 0 ' O 3' 'atom/o3_28+13lev.dat'
8 3 39 0 0 0 ' O 4' 'atom/o4_31+8lev.dat'
8 4 6 0 0 0 ' O 5' 'atom/o5_34+6lev.dat'
8 5 1 1 0 0 ' O 6' ' '
10 0 35 0 0 0 'Ne 1' 'atom/ne1_23+12lev.dat'
10 1 32 0 0 0 'Ne 2' 'atom/ne2_23+9lev.dat'
10 2 34 0 0 0 'Ne 3' 'atom/ne3_22+12lev.dat'
10 3 12 0 0 0 'Ne 4' 'atom/ne4_10+2lev.dat'
10 4 1 1 0 0 'Ne 5' ' '
12 1 25 0 0 0 'Mg 2' 'atom/mg2_21+4lev.dat'
12 2 1 1 0 0 'Mg 3' ' '
13 1 29 0 0 0 'Al 2' 'atom/al2_20+9lev.dat'
13 2 23 0 0 0 'Al 3' 'atom/al3_19+4lev.dat'
13 3 1 1 0 0 'Al 4' ' '
14 1 40 0 0 0 'Si 2' 'atom/si2_36+4lev.dat'
14 2 30 0 0 0 'Si 3' 'atom/si3_24+6lev.dat'
14 3 23 0 0 0 'Si 4' 'atom/si4_19+4lev.dat'
14 4 1 1 0 0 'Si 5' ' '
16 1 33 0 0 0 ' S 2' 'atom/s2_23+10lev.dat'
16 2 41 0 0 0 ' S 3' 'atom/s3_29+12lev.dat'
16 3 38 0 0 0 ' S 4' 'atom/s4_33+5lev.dat'
16 4 25 0 0 0 ' S 5' 'atom/s5_20+5lev.dat'
16 5 1 1 0 0 ' S 6' ' '
26 1 36 0 0 -1 'Fe 2' 'atom/fe2v.dat'
0 0 'atom/gf2601.gam'
'atom/gf2601.lin'
'atom/fe2p_14+11lev.rap'
26 2 50 0 0 -1 'Fe 3' 'atom/fe3v.dat'
0 0 'atom/gf2602.gam'
'atom/gf2602.lin'
'atom/fe3p_22+7lev.rap'
26 3 43 0 0 -1 'Fe 4' 'atom/fe4v.dat'
0 0 'atom/gf2603.gam'
'atom/gf2603.lin'
'atom/fe4p_21+11lev.rap'
26 4 42 0 0 -1 'Fe 5' 'atom/fe5v.dat'
0 0 'atom/gf2604.gam'
'atom/gf2604.lin'
'atom/fe5p_19+11lev.rap'
26 5 1 1 0 0 'Fe 6' ' '
0 0 0 -1 0 0 ' ' ' '
*
* end
File diff suppressed because it is too large Load Diff
+5
View File
@@ -0,0 +1,5 @@
NLAMBD=3,ITEK=4,XGRAD=-1.,
NITER=31,ND=50,VTB=2.,
ISPODF=1,STRLX=1.D-10,DDNU=0.75,
ICOLHN=1,ITLAS=0,
POPZER=1.D-30,POPZR2=1.D-30
+964
View File
@@ -0,0 +1,964 @@
****** Levels
4.55265084E+15 1. 3 'AlII 1Se 1' 0 0. 0
3.42794359E+15 9. 3 'AlII 3Po 1' 0 0. 0
2.75835282E+15 3. 3 'AlII 1Po 1' 0 0. 0
1.99001981E+15 5. 4 'AlII 1De 1' 0 0. -104
1.81634905E+15 3. 4 'AlII 3Se 1' 0 0. -104
1.72841389E+15 9. 4 'AlII 3Pe 1' 0 0. -104
1.69415414E+15 1. 4 'AlII 1Se 2' 0 0. -104
1.68817005E+15 15. 4 'AlII 3De 1' 0 0. -104
1.39119883E+15 9. 4 'AlII 3Po 2' 0 0. -104
1.34730359E+15 3. 4 'AlII 1Po 2' 0 0. -104
1.25229462E+15 5. 4 'AlII 1De 2' 0 0. -104
1.20590226E+15 1. 4 'AlII 1Se 3' 0 0. -104
9.52415507E+14 3. 5 'AlII 3Se 2' 0 0. -104
9.14228014E+14 1. 5 'AlII 1Se 4' 0 0. -104
9.10717616E+14 15. 5 'AlII 3De 2' 0 0. -104
8.52636840E+14 21. 5 'AlII 3Fo 1' 0 0. -104
8.51159640E+14 7. 5 'AlII 1Fo 1' 0 0. -104
8.11478370E+14 5. 5 'AlII 1De 3' 0 0. -104
7.83860657E+14 9. 5 'AlII 3Po 3' 0 0. -104
7.79255110E+14 3. 5 'AlII 1Po 3' 0 0. -104
5.45297738E+14 75. 6 'AlII+3__ 1' 0 0. -104
5.35428944E+14 25. 6 'AlII+1__ 2' 0 0. -104
3.81736089E+14 108. 7 'AlII+3__ 3' 0 0. -104
3.72560596E+14 36. 7 'AlII+1__ 4' 0 0. -104
2.89005598E+14 147. 8 'AlII+3__ 5' 0 0. -104
2.73499306E+14 49. 8 'AlII+1__ 6' 0 0. -104
2.20838863E+14 256. 9 'AlII+___ 7' 0 0. -104
1.75416564E+14 324. 10 'AlII+___ 8' 0 0. -104
1.42483879E+14 400. 11 'AlII+___ 9' 0 0. -104
****** Continuum transitions
1 30 1 122 0 0 0 4.128E-20 0.000E+00
-0.0127 -0.0062 0.0067 0.0132 0.0196 0.0261 0.0326 0.0455 0.0520 0.0584
0.0713 0.0843 0.1489 0.1619 0.2071 0.2783 0.4011 0.4722 0.5110 0.5498
0.5757 1.1855
-0.4242 -0.5474 -0.8329 -0.8754 -0.8953 -0.8318 -0.7375 -0.5884 -0.5477 -0.5412
-0.5693 -0.5596 -0.4812 -0.4732 -0.4840 -0.4834 -0.5354 -0.5981 -0.6157 -0.6675
-0.7286 -2.5591
2 30 1 120 0 0 0 1.327E-19 0.000E+00
-0.0169 0.0154 0.0219 0.0283 0.0348 0.0607 0.0736 0.0930 0.1124 0.1318
0.1577 0.1835 0.2417 0.2805 0.3646 0.3969 0.7331 0.7655 0.9336 1.4045
-0.1410 -0.2122 -0.2120 -0.2221 -0.2477 -0.4074 -0.4273 -0.4348 -0.4723 -0.4705
-0.4492 -0.4534 -0.4025 -0.3952 -0.3857 -0.3984 -0.6288 -0.6873 -1.1864 -2.6017
3 30 1 140 0 0 0 5.475E-19 0.000E+00
-0.0214 -0.0020 0.0044 0.0303 0.0368 0.0432 0.0497 0.0562 0.0626 0.0691
0.0756 0.0820 0.0950 0.1144 0.1208 0.1402 0.1532 0.1596 0.1661 0.1726
0.1790 0.1920 0.1984 0.2049 0.2114 0.2372 0.2437 0.2502 0.2696 0.2760
0.3083 0.3342 0.3989 0.4635 0.6381 0.7480 0.7998 0.8450 0.8644 1.4628
0.5661 0.4583 0.3913 0.0709 -0.0014 -0.0281 0.0167 0.0771 0.1170 0.1236
0.0962 0.0504 -0.0797 -0.3002 -0.3482 -0.4586 -0.5506 -0.5871 -0.6104 -0.6050
-0.5651 -0.4312 -0.3841 -0.3713 -0.3894 -0.5672 -0.5997 -0.6003 -0.5536 -0.5280
-0.4732 -0.4930 -0.4612 -0.4615 -0.5251 -0.6139 -0.6646 -0.6960 -0.7386 -2.5345
4 30 1 147 0 0 0 2.875E-18 0.000E+00
-0.0295 -0.0231 -0.0166 0.0028 0.0222 0.0351 0.0416 0.0481 0.0545 0.0610
0.0675 0.0739 0.0804 0.0933 0.1127 0.1192 0.1257 0.1321 0.1386 0.1450
0.1580 0.1644 0.1709 0.1774 0.1838 0.1903 0.2032 0.2614 0.2744 0.2808
0.2938 0.3067 0.3132 0.3261 0.3390 0.3455 0.3584 0.3714 0.3843 0.4037
0.4360 0.4942 0.5524 0.8498 0.9662 0.9986 1.5987
1.3425 1.3190 1.2843 1.1362 1.0254 0.9581 0.8960 0.8034 0.6701 0.4937
0.2969 0.1430 0.1394 0.3252 0.6542 0.7405 0.7957 0.8082 0.7646 0.6838
0.4236 0.3602 0.3800 0.4220 0.4318 0.3998 0.2981 -0.0174 -0.0706 -0.0938
-0.0899 -0.0691 -0.0778 -0.1446 -0.2393 -0.2717 -0.2846 -0.2931 -0.3216 -0.3333
-0.3452 -0.3801 -0.4007 -0.5932 -0.7163 -0.8018 -2.6047
5 30 1 160 0 0 0 1.302E-18 0.000E+00
-0.0327 -0.0198 -0.0133 -0.0068 -0.0004 0.0061 0.0126 0.0190 0.0255 0.0320
0.0384 0.0449 0.0514 0.0578 0.0643 0.0708 0.0837 0.1096 0.1160 0.1225
0.1290 0.1354 0.1419 0.1484 0.1548 0.1678 0.1742 0.1872 0.1936 0.2066
0.2260 0.2518 0.2583 0.2712 0.2971 0.3165 0.3229 0.3294 0.3359 0.3423
0.3553 0.3617 0.3876 0.3941 0.4070 0.4135 0.4199 0.4329 0.4393 0.4652
0.4846 0.5751 0.7174 0.7820 0.8467 0.8855 0.9437 1.0019 1.0277 1.5847
0.6898 0.8677 0.9218 0.9120 0.8234 0.6468 0.3864 0.0470 -0.3569 -0.8056
-1.2690 -1.6999 -2.0009 -2.0556 -1.9299 -1.7828 -1.5123 -1.0554 -0.8933 -0.7441
-0.6361 -0.6031 -0.6443 -0.7431 -0.8631 -0.9589 -0.9257 -0.8300 -0.8053 -0.8064
-0.7804 -0.7689 -0.7594 -0.7089 -0.5913 -0.1234 -0.0256 -0.0087 -0.0744 -0.2148
-0.5885 -0.6913 -0.7380 -0.6834 -0.5033 -0.4610 -0.4649 -0.5155 -0.5164 -0.4839
-0.4695 -0.4851 -0.5549 -0.6163 -0.6633 -0.7073 -0.7439 -0.8169 -0.8789 -2.5516
6 30 1 165 0 0 0 1.664E-17 0.000E+00
-0.0348 -0.0283 -0.0219 -0.0154 -0.0089 -0.0025 0.0040 0.0105 0.0169 0.0234
0.0299 0.0363 0.0428 0.0493 0.0557 0.0622 0.0687 0.0816 0.0945 0.1010
0.1075 0.1139 0.1204 0.1269 0.1333 0.1398 0.1463 0.1527 0.1592 0.1657
0.1721 0.1786 0.1851 0.1915 0.1980 0.2045 0.2109 0.2174 0.2239 0.2368
0.2497 0.2562 0.2627 0.2691 0.2756 0.2950 0.3014 0.3273 0.3467 0.3661
0.3920 0.4178 0.4372 0.4825 0.5213 0.5472 0.5730 0.6054 0.8252 0.9028
0.9674 1.0127 1.0321 1.1226 1.6342
1.5530 1.7626 1.9286 2.0298 2.0514 1.9818 1.8194 1.5666 1.2257 0.8045
0.3183 -0.1855 -0.6293 -0.9265 -1.0994 -1.1735 -1.2339 -1.2858 -1.2568 -1.0614
-0.8059 -0.3699 0.0482 0.3822 0.6138 0.7356 0.7542 0.6745 0.5024 0.2451
-0.0648 -0.2858 -0.2392 -0.0316 0.1270 0.1933 0.1817 0.1319 0.0934 0.0676
0.0029 -0.0112 0.0095 0.0535 0.0837 0.0947 0.0869 -0.0309 -0.0939 -0.1774
-0.2729 -0.3142 -0.3359 -0.3541 -0.3311 -0.3263 -0.2982 -0.3013 -0.3880 -0.4571
-0.5259 -0.5587 -0.5932 -0.8588 -2.3961
7 30 1 166 0 0 0 1.258E-17 0.000E+00
-0.0352 -0.0288 -0.0223 -0.0158 -0.0094 -0.0029 0.0036 0.0230 0.0359 0.0424
0.0488 0.0618 0.0747 0.0812 0.0941 0.1006 0.1135 0.1200 0.1264 0.1329
0.1394 0.1458 0.1523 0.1588 0.1652 0.1717 0.1782 0.1846 0.1911 0.1976
0.2040 0.2105 0.2170 0.2234 0.2299 0.2428 0.2816 0.3204 0.3398 0.3463
0.3527 0.3786 0.3851 0.3915 0.4109 0.4174 0.4239 0.4303 0.4368 0.4433
0.4562 0.4627 0.4691 0.4821 0.4885 0.5209 0.5920 0.6502 0.7472 0.8054
0.8765 0.9347 0.9929 1.0317 1.0640 1.6129
2.2016 2.1823 2.1450 2.0763 1.9883 1.8658 1.7156 1.2045 0.8860 0.7395
0.6028 0.3571 0.1322 0.0108 -0.2598 -0.4083 -0.7265 -0.8489 -0.8479 -0.6978
-0.5241 -0.4128 -0.3887 -0.4497 -0.5940 -0.8067 -1.0495 -1.1993 -1.1384 -0.9924
-0.8925 -0.8690 -0.9044 -0.9565 -0.9854 -0.9822 -0.9621 -0.9167 -0.8527 -0.8382
-0.8366 -0.8671 -0.8805 -0.9034 -0.8875 -0.7874 -0.6673 -0.5627 -0.5057 -0.4906
-0.5009 -0.5155 -0.5468 -0.6211 -0.6344 -0.6146 -0.5542 -0.5567 -0.5975 -0.6462
-0.6878 -0.7452 -0.7822 -0.8238 -0.9096 -2.5586
8 30 1 143 0 0 0 1.306E-17 0.000E+00
-0.0352 -0.0223 -0.0158 -0.0093 -0.0029 0.0036 0.0101 0.0230 0.0295 0.0553
0.0877 0.1329 0.1394 0.1458 0.1523 0.1588 0.1652 0.1717 0.1976 0.2170
0.2881 0.3140 0.3334 0.3398 0.3528 0.3722 0.3980 0.4045 0.4110 0.4304
0.4368 0.4562 0.4627 0.4756 0.5015 0.5209 0.5532 0.7149 0.8377 0.9153
0.9670 1.0058 1.5551
1.6330 1.8307 1.9036 1.9187 1.8675 1.7491 1.5872 1.3176 1.1894 1.0437
0.9194 0.8063 0.7680 0.7098 0.6425 0.5916 0.5594 0.5360 0.4988 0.4101
0.1876 0.1154 0.0892 0.0689 -0.0065 -0.0640 -0.1278 -0.1238 -0.1332 -0.2150
-0.2282 -0.2349 -0.2464 -0.2907 -0.3458 -0.3601 -0.4148 -0.6054 -0.7369 -0.8223
-0.8593 -0.9343 -2.5814
9 30 1 167 0 0 0 3.032E-19 0.000E+00
-0.0433 -0.0239 -0.0110 -0.0045 0.0020 0.0084 0.0149 0.0214 0.0278 0.0343
0.0407 0.0472 0.0537 0.0601 0.0666 0.0731 0.0795 0.0860 0.0925 0.0989
0.1054 0.1119 0.1183 0.1248 0.1313 0.1377 0.1571 0.1895 0.2089 0.2541
0.2994 0.3123 0.3382 0.3447 0.3511 0.3576 0.4222 0.4287 0.4416 0.4481
0.4546 0.4610 0.4675 0.4740 0.4804 0.4934 0.4998 0.5063 0.5128 0.5192
0.5257 0.5322 0.5386 0.5451 0.5580 0.5645 0.5774 0.6292 0.7003 0.8425
0.9007 0.9460 1.0107 1.0624 1.1141 1.1917 1.7000
0.1793 0.1345 0.1246 0.1444 0.1964 0.3202 0.5356 0.8538 1.2056 1.5258
1.7787 1.9485 2.0380 2.0579 2.0229 1.9488 1.8399 1.6867 1.4843 1.2368
0.9669 0.7331 0.5413 0.4148 0.3313 0.2613 0.1118 -0.0917 -0.2028 -0.4173
-0.5617 -0.5887 -0.5877 -0.5982 -0.6176 -0.6459 -0.7770 -0.7472 -0.6256 -0.5183
-0.4217 -0.3642 -0.3616 -0.4176 -0.5274 -0.7632 -0.8184 -0.8489 -0.8048 -0.7046
-0.5764 -0.4672 -0.4084 -0.4062 -0.4913 -0.5184 -0.5237 -0.5209 -0.5377 -0.5885
-0.6429 -0.6678 -0.7391 -0.7741 -0.8490 -1.0754 -2.6028
10 30 1 177 0 0 0 3.0025E-19 0.000E+00
-0.0451 -0.0192 -0.0128 -0.0063 0.0002 0.0066 0.0131 0.0196 0.0260 0.0325
0.0390 0.0454 0.0519 0.0713 0.0777 0.0842 0.0907 0.0971 0.1036 0.1101
0.1165 0.1230 0.1295 0.1359 0.1553 0.1618 0.1683 0.1877 0.1941 0.2006
0.2071 0.2200 0.2265 0.2329 0.2523 0.2588 0.2717 0.3105 0.3170 0.3235
0.3299 0.3364 0.3429 0.3493 0.3558 0.3623 0.3687 0.3752 0.3946 0.4010
0.4269 0.4334 0.4463 0.4592 0.4657 0.4722 0.4786 0.4916 0.4980 0.5045
0.5174 0.5239 0.5304 0.5433 0.5498 0.5562 0.5692 0.5756 0.6015 0.6920
0.8278 0.9313 0.9830 1.0671 1.1252 1.1576 1.7068
0.2234 0.1598 0.1522 0.1558 0.1769 0.2095 0.2693 0.3398 0.4278 0.5321
0.6469 0.7733 0.9141 1.3745 1.5146 1.6280 1.7127 1.7639 1.7784 1.7631
1.7227 1.6547 1.5565 1.4259 0.9794 0.8568 0.7438 0.4456 0.3576 0.2929
0.2593 0.3130 0.3178 0.2822 0.0884 0.0329 -0.0177 -0.2151 -0.2433 -0.2611
-0.2464 -0.2131 -0.1644 -0.1262 -0.1293 -0.1911 -0.3139 -0.4543 -0.7052 -0.7407
-0.7616 -0.7312 -0.5916 -0.3790 -0.3250 -0.3262 -0.3684 -0.4682 -0.5074 -0.5579
-0.6854 -0.7110 -0.6767 -0.5334 -0.5028 -0.5176 -0.5927 -0.5988 -0.5544 -0.5407
-0.5490 -0.6280 -0.6602 -0.7564 -0.8147 -0.9003 -2.5505
11 30 1 169 0 0 0 5.484E-18 0.000E+00
-0.0489 -0.0230 -0.0166 -0.0036 0.0093 0.0222 0.0352 0.0546 0.0675 0.0740
0.0804 0.0869 0.0934 0.0998 0.1063 0.1128 0.1192 0.1322 0.1580 0.1645
0.1710 0.1774 0.1839 0.1968 0.2033 0.2098 0.2162 0.2227 0.2292 0.2356
0.2485 0.2550 0.2615 0.2679 0.2744 0.2809 0.2938 0.3326 0.3455 0.3779
0.3908 0.4102 0.4296 0.4361 0.4555 0.4749 0.4943 0.5137 0.5266 0.5331
0.5395 0.5589 0.5654 0.5719 0.5783 0.5912 0.5977 0.6042 0.6171 0.6236
0.6300 0.6430 0.6494 0.6818 0.7076 1.0956 1.1538 1.1797 1.8070
1.3395 1.3614 1.3697 1.4149 1.4975 1.6065 1.7364 1.9450 2.0631 2.0940
2.1149 2.1094 2.0708 2.0145 1.9438 1.8509 1.7412 1.4986 0.9938 0.8816
0.7932 0.7352 0.7092 0.6752 0.6736 0.7009 0.7378 0.7556 0.7233 0.6599
0.4741 0.4392 0.4657 0.5079 0.5233 0.5019 0.4231 0.3061 0.2687 0.1189
0.0346 -0.1022 -0.2766 -0.3121 -0.3515 -0.3769 -0.3768 -0.4475 -0.4636 -0.4621
-0.4508 -0.3871 -0.3836 -0.4037 -0.4491 -0.5597 -0.5833 -0.5708 -0.4909 -0.4630
-0.4592 -0.4934 -0.5013 -0.4611 -0.4667 -0.7027 -0.7709 -0.8350 -2.7190
12 30 1 187 0 0 0 6.236E-19 0.000E+00
-0.0526 -0.0396 -0.0332 -0.0267 -0.0202 -0.0138 -0.0073 -0.0008 0.0186 0.0315
0.0380 0.0444 0.0509 0.0574 0.0638 0.0703 0.0768 0.0832 0.0897 0.0962
0.1026 0.1091 0.1156 0.1220 0.1285 0.1350 0.1414 0.1479 0.1544 0.1608
0.1738 0.1802 0.1867 0.1932 0.2061 0.2190 0.2255 0.2320 0.2384 0.2449
0.2514 0.2578 0.2643 0.2708 0.2772 0.2837 0.2901 0.2966 0.3031 0.3095
0.3160 0.3225 0.3419 0.3483 0.3548 0.3613 0.4001 0.4259 0.4389 0.4453
0.4583 0.4712 0.4777 0.4841 0.4906 0.4971 0.5035 0.5100 0.5165 0.5423
0.5617 0.5811 0.6005 0.6199 0.6522 0.6652 0.6781 0.7040 0.7169 0.7686
0.8980 1.0273 1.1049 1.1437 1.1825 1.2083 1.7391
0.9968 0.9892 0.9657 0.9155 0.8489 0.7590 0.6462 0.5181 0.0931 -0.2017
-0.3559 -0.5002 -0.5294 -0.3093 0.0867 0.4466 0.7070 0.8571 0.9043 0.8500
0.7021 0.4663 0.1555 -0.2097 -0.5982 -0.9740 -1.3061 -1.5421 -1.5374 -1.2304
-0.3955 -0.0316 0.2646 0.4877 0.8247 1.2085 1.3474 1.4003 1.3564 1.2142
0.9841 0.7222 0.6060 0.7366 0.9177 1.0283 1.0477 0.9815 0.8599 0.7293
0.6495 0.6379 0.7262 0.7421 0.7462 0.7348 0.4790 0.2927 0.2219 0.2047
0.2103 0.1877 0.1513 0.0827 -0.0168 -0.1280 -0.2221 -0.2749 -0.3121 -0.3370
-0.3881 -0.4051 -0.4380 -0.4432 -0.4120 -0.4100 -0.3858 -0.2929 -0.2722 -0.2667
-0.3756 -0.4633 -0.5355 -0.5827 -0.6169 -0.6794 -2.2736
13 30 1 189 0 0 0 7.446E-20 0.000E+00
-0.0648 -0.0519 -0.0454 -0.0390 -0.0325 -0.0260 -0.0196 -0.0131 -0.0066 -0.0002
0.0063 0.0128 0.0192 0.0322 0.0451 0.1227 0.1356 0.1550 0.1679 0.1744
0.1809 0.1873 0.1938 0.2003 0.2067 0.2132 0.2197 0.2261 0.2326 0.2391
0.2455 0.2520 0.2585 0.2649 0.2714 0.2843 0.2908 0.2973 0.3037 0.3102
0.3167 0.3231 0.3296 0.3361 0.3425 0.3490 0.3555 0.3619 0.3684 0.3813
0.3878 0.3942 0.4201 0.4912 0.5106 0.5236 0.5300 0.5753 0.5818 0.5947
0.6012 0.6141 0.6206 0.6335 0.6400 0.6464 0.6529 0.6594 0.6658 0.6723
0.6788 0.6852 0.6917 0.6982 0.7046 0.7111 0.7305 0.7434 0.7628 0.7757
0.8145 0.8857 0.9568 1.0279 1.0538 1.0926 1.1378 1.1702 1.6945
-1.2203 -0.9633 -0.7580 -0.5253 -0.3171 -0.1714 -0.1074 -0.1309 -0.2396 -0.4229
-0.6481 -0.8464 -0.9186 -0.9272 -0.8692 -0.4765 -0.4139 -0.2922 -0.1810 -0.1031
-0.0016 0.2116 0.5253 0.9924 1.4409 1.8127 2.0716 2.2210 2.2633 2.2022
2.0412 1.7891 1.4481 1.0288 0.5445 -0.5096 -0.9688 -1.2366 -1.2494 -1.1423
-1.0758 -1.0938 -1.1920 -1.3234 -1.3900 -1.3663 -1.3135 -1.2981 -1.3241 -1.3961
-1.4113 -1.4156 -1.3896 -1.3593 -1.3777 -1.3933 -1.3879 -1.2559 -1.2037 -1.0445
-0.9721 -0.8810 -0.7676 -0.3533 -0.1999 -0.1330 -0.1593 -0.2779 -0.4802 -0.7354
-1.0001 -1.1879 -1.2756 -1.3150 -1.3434 -1.3595 -1.3576 -1.4053 -1.4871 -1.5258
-1.5870 -1.6733 -1.7430 -1.8542 -1.8777 -1.9027 -1.9778 -2.0604 -3.6353
14 30 1 188 0 0 0 2.218E-19 0.000E+00
-0.0676 -0.0611 -0.0546 -0.0482 -0.0417 -0.0288 -0.0223 -0.0158 -0.0094 -0.0029
0.0036 0.0100 0.0165 0.0230 0.0294 0.0359 0.0553 0.0618 0.1006 0.1135
0.1264 0.1458 0.1588 0.1717 0.1846 0.1911 0.1976 0.2040 0.2105 0.2234
0.2299 0.2363 0.2428 0.2493 0.2557 0.2622 0.2687 0.2751 0.2881 0.2945
0.3010 0.3075 0.3139 0.3204 0.3269 0.3398 0.3463 0.3592 0.3657 0.3721
0.3851 0.3980 0.4174 0.4433 0.4756 0.5079 0.5597 0.5726 0.5855 0.5920
0.5984 0.6049 0.6178 0.6308 0.6372 0.6502 0.6566 0.6631 0.6696 0.6760
0.6825 0.6890 0.6954 0.7084 0.7148 0.7213 0.7278 0.7342 0.7472 0.7601
0.7730 0.7924 0.8183 0.9088 0.9670 1.0446 1.0705 1.6722
1.1374 1.1278 1.1084 1.0742 1.0198 0.8355 0.7035 0.5437 0.3590 0.1498
-0.0842 -0.3433 -0.6221 -0.8765 -1.0151 -0.9641 -0.5313 -0.4387 0.0295 0.1575
0.2549 0.3914 0.4908 0.6128 0.7631 0.8602 0.9734 1.1291 1.3356 1.8159
2.0191 2.1594 2.2186 2.2047 2.1110 1.9448 1.7205 1.4552 0.8946 0.6313
0.3895 0.1711 -0.0143 -0.1533 -0.2594 -0.3761 -0.4688 -0.6887 -0.7884 -0.8602
-0.9827 -1.0841 -1.2036 -1.3169 -1.3946 -1.4108 -1.3453 -1.3435 -1.3226 -1.2956
-1.2431 -1.1535 -0.9371 -0.7893 -0.6912 -0.4419 -0.3569 -0.3203 -0.3302 -0.3799
-0.4611 -0.5656 -0.6866 -0.9533 -1.0755 -1.1723 -1.2316 -1.2606 -1.2870 -1.3358
-1.3929 -1.4468 -1.4811 -1.5567 -1.5848 -1.7116 -1.7706 -3.5769
15 30 1 156 0 0 0 2.422E-18 0.000E+00
-0.0681 -0.0164 0.0806 0.1259 0.1323 0.1841 0.1905 0.2035 0.2099 0.2164
0.2229 0.2293 0.2358 0.2423 0.2487 0.2552 0.2617 0.2746 0.2811 0.2875
0.3005 0.3199 0.3263 0.3392 0.3457 0.4039 0.4556 0.4686 0.5009 0.5138
0.5526 0.5914 0.6173 0.6238 0.6302 0.6367 0.6496 0.6561 0.6626 0.6690
0.6755 0.6819 0.6884 0.7013 0.7078 0.7272 0.7595 0.8048 0.8630 1.0053
1.0699 1.1346 1.1992 1.2510 1.2898 1.8292
1.2075 1.1330 0.8379 0.6818 0.6526 0.3049 0.3234 0.4281 0.7238 1.1394
1.4858 1.7314 1.8770 1.9279 1.8978 1.7948 1.6358 1.2401 1.0745 0.9345
0.7830 0.6934 0.6496 0.5300 0.4806 0.2464 0.0731 0.0388 -0.0269 -0.0302
-0.1489 -0.2534 -0.3381 -0.3538 -0.3467 -0.2996 -0.1902 -0.1698 -0.1951 -0.2618
-0.3497 -0.4164 -0.4558 -0.4456 -0.4496 -0.4884 -0.5450 -0.5873 -0.6608 -0.7512
-0.8213 -0.8668 -0.9480 -0.9818 -1.0606 -2.6792
16 30 1 187 0 0 0 1.096E-18 0.000E+00
-0.0727 -0.0339 0.0372 0.0566 0.0631 0.0695 0.0760 0.0825 0.0889 0.0954
0.1019 0.1213 0.1277 0.1536 0.1730 0.1989 0.2118 0.2183 0.2247 0.2312
0.2377 0.2441 0.2571 0.2635 0.2700 0.2765 0.2829 0.2894 0.2959 0.3023
0.3088 0.3153 0.3217 0.3282 0.3347 0.3411 0.3476 0.3540 0.3605 0.3864
0.3993 0.4187 0.4252 0.4316 0.4381 0.4510 0.4575 0.4640 0.4704 0.4834
0.5092 0.5480 0.5545 0.5739 0.5868 0.5933 0.5998 0.6192 0.6386 0.6450
0.6515 0.6580 0.6644 0.6709 0.6774 0.6838 0.6903 0.6967 0.7032 0.7161
0.7226 0.7291 0.7355 0.7420 0.7485 0.7614 0.7679 0.7743 0.8002 0.8390
0.9295 1.0588 1.1946 1.2334 1.2722 1.3110 1.8801
0.9869 0.8777 0.5862 0.5430 0.5487 0.5853 0.6390 0.6804 0.6905 0.6600
0.5968 0.3541 0.2889 0.0857 -0.0589 -0.3056 -0.4627 -0.5345 -0.5962 -0.5700
-0.3864 -0.0228 0.8790 1.2616 1.5595 1.7626 1.8689 1.8843 1.8105 1.6542
1.4302 1.1629 0.8857 0.6489 0.4734 0.3234 0.2217 0.1344 0.0756 -0.0754
-0.1538 -0.2476 -0.2694 -0.2711 -0.2484 -0.1815 -0.1760 -0.2055 -0.2701 -0.4482
-0.6431 -0.7871 -0.7999 -0.7855 -0.7291 -0.7333 -0.7731 -0.9498 -1.0662 -1.0785
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17 30 1 175 0 0 0 1.047E-18 0.000E+00
-0.0729 -0.0341 0.0370 0.0888 0.1405 0.1534 0.1599 0.1857 0.1987 0.2116
0.2181 0.2245 0.2310 0.2375 0.2504 0.2569 0.2633 0.2698 0.2763 0.2827
0.2892 0.2957 0.3021 0.3086 0.3215 0.3280 0.3345 0.3409 0.3474 0.3539
0.3603 0.3991 0.4185 0.4379 0.4638 0.5090 0.5608 0.5672 0.5931 0.5996
0.6060 0.6125 0.6190 0.6254 0.6319 0.6384 0.6448 0.6513 0.6578 0.6642
0.6707 0.6772 0.6836 0.6901 0.6966 0.7030 0.7095 0.7160 0.7224 0.7289
0.7354 0.7418 0.7548 0.7612 0.7677 0.7806 0.7871 0.8324 0.9293 1.0587
1.1944 1.2268 1.2785 1.3108 1.8811
0.9709 0.8602 0.5651 0.3219 0.0546 -0.0174 -0.0626 -0.3103 -0.4992 -0.7253
-0.8284 -0.8282 -0.6388 -0.2654 0.6641 1.0881 1.4394 1.7034 1.8761 1.9579
1.9500 1.8559 1.6841 1.4434 0.8788 0.6439 0.4649 0.3298 0.2145 0.1348
0.0798 -0.1753 -0.2806 -0.3581 -0.4108 -0.6093 -0.8816 -0.9033 -0.9162 -0.9360
-0.9738 -1.0007 -1.0108 -1.0069 -0.9834 -0.9764 -0.9867 -0.9673 -0.8574 -0.6709
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18 30 1 187 0 0 0 5.612E-19 0.000E+00
-0.0783 -0.0589 -0.0525 -0.0460 -0.0266 -0.0137 -0.0072 -0.0007 0.0057 0.0122
0.0187 0.0251 0.0316 0.0445 0.0833 0.0898 0.1157 0.1221 0.1286 0.1351
0.1609 0.1674 0.1803 0.1868 0.1932 0.1997 0.2062 0.2126 0.2191 0.2256
0.2320 0.2385 0.2450 0.2579 0.2644 0.2708 0.2773 0.2838 0.2902 0.2967
0.3032 0.3096 0.3161 0.3226 0.3290 0.3549 0.3614 0.3678 0.3743 0.3872
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0.6695 0.6759 0.6824 0.6889 0.6953 0.7018 0.7083 0.7147 0.7212 0.7277
0.7341 0.7406 0.7471 0.7535 0.7665 0.7729 0.7794 0.7859 0.7923 0.7988
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28 30 1 115 0 0 0 3.212E-19 0.000E+00
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29 30 1 114 0 0 0 4.143E-19 0.000E+00
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-2.373 -2.708 -3.025 -4.891
*** Line transitions
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1 3 -1 1 1 0 0 1.840E+00 7.000E-01
T 3 29 1000. 0.
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9 10 0 0 4 0 0 0.000E+00 5.000E-02
9 11 0 0 4 0 0 0.000E+00 5.000E-02
9 12 0 0 4 0 0 0.000E+00 5.000E-02
9 13 -1 0 1 0 0 2.500E-01 2.000E-01
F 1 7 0. 0.
9 14 0 0 4 0 0 0.000E+00 5.000E-02
9 15 -1 0 1 0 0 1.086E+00 2.000E-01
F 1 7 0. 0.
9 16 0 0 4 0 0 0.000E+00 5.000E-02
9 17 0 0 4 0 0 0.000E+00 5.000E-02
9 18 0 0 4 0 0 0.000E+00 5.000E-02
9 19 0 0 4 0 0 0.000E+00 5.000E-02
9 20 0 0 4 0 0 0.000E+00 5.000E-02
9 21 -1 0 1 0 0 1.060E-01 2.000E-01
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9 23 -1 0 1 0 0 2.721E-02 2.000E-01
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9 24 0 0 4 0 0 0.000E+00 5.000E-02
9 25 -1 0 1 0 0 1.071E-02 2.000E-01
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9 27 -1 0 1 0 0 5.256E-03 2.000E-01
F 1 7 0. 0.
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10 14 -1 0 1 0 0 2.373E-01 2.000E-01
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10 15 0 0 4 0 0 0.000E+00 5.000E-02
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10 17 0 0 4 0 0 0.000E+00 5.000E-02
10 18 -1 0 1 0 0 6.867E-01 2.000E-01
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11 13 0 0 4 0 0 0.000E+00 5.000E-02
11 14 0 0 4 0 0 0.000E+00 5.000E-02
11 15 0 0 4 0 0 0.000E+00 5.000E-02
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11 17 -1 0 1 0 0 6.260E-01 2.000E-01
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12 24 -1 0 1 0 0 3.700E-03 2.000E-01
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13 16 0 0 4 0 0 0.000E+00 5.000E-02
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+501
View File
@@ -0,0 +1,501 @@
****** Levels
6.87845401E+15 2. 3 'Al+2 2Se 1' 0 0. 0
5.26923650E+15 2. 3 'Al+2 2Po 1' 0 0. 0
5.26223070E+15 4. 3 'Al+2 2Po 1' 0 0. 0
3.40221754E+15 10. 3 'Al+2 2De 1' 0 0. 0
3.09624192E+15 2. 4 'Al+2 2Se 2' 0 0. -105
2.57093441E+15 6. 4 'Al+2 2Po 2' 0 0. -105
1.90840698E+15 10. 4 'Al+2 2De 2' 0 0. -105
1.85365554E+15 14. 4 'Al+2 2Fo 1' 0 0. -105
1.76299267E+15 2. 5 'Al+2 2Se 3' 0 0. -105
1.52854034E+15 6. 5 'Al+2 2Po 3' 0 0. -105
1.21617019E+15 10. 5 'Al+2 2De 3' 0 0. -105
1.18623628E+15 14. 5 'Al+2 2Fo 2' 0 0. -105
1.18466660E+15 18. 5 'Al+2 2Ge 1' 0 0. -105
1.13803104E+15 2. 6 'Al+2 2Se 4' 0 0. -105
1.01359564E+15 6. 6 'Al+2 2Po 4' 0 0. -105
8.41510526E+14 10. 6 'Al+2 2De 4' 0 0. -105
8.23650375E+14 14. 6 'Al+2 2Fo 3' 0 0. -105
8.22676558E+14 18. 6 'Al+2 2Ge 2' 0 0. -105
8.22492478E+14 22. 6 'Al+2 2Ho 1' 0 0. -105
6.20337696E+14 98. 7 'Al+2+2__ 1' 0 0. -105
4.69959415E+14 128. 8 'Al+2+2__ 2' 0 0. -105
3.69310648E+14 162. 9 'Al+2+2__ 3' 0 0. -105
2.98370371E+14 200. 10 'Al+2+2__ 4' 0 0. -105
****** Continuum transitions
1 24 1 105 0 0 0 6.051E-20 0.000E+00
-0.0193 0.0583 0.1747 0.2846 0.3621
-0.5121 -0.5406 -0.6212 -0.7283 -0.8228
2 24 1 107 0 0 0 8.542E-20 0.000E+00
-0.0254 0.1104 0.2009 0.2850 0.3497 0.4208 0.4317
-0.3692 -0.3708 -0.4005 -0.4593 -0.5312 -0.6335 -0.6505
3 24 1 107 0 0 0 8.542E-20 0.000E+00
-0.0254 0.1104 0.2009 0.2850 0.3497 0.4208 0.4317
-0.3692 -0.3708 -0.4005 -0.4593 -0.5312 -0.6335 -0.6505
4 24 1 111 0 0 0 5.160E-19 0.000E+00
-0.0394 -0.0200 0.0252 0.1869 0.4649 0.5878 0.6524 0.6977 0.7300 0.7688
0.7929
0.5048 0.4708 0.3371 -0.1933 -1.1543 -1.5852 -1.8352 -2.0383 -2.2026 -2.4443
-2.6064
5 24 1 106 0 0 0 7.187E-20 0.000E+00
-0.0439 0.0208 0.1177 0.2471 0.4281 0.5893
-0.4271 -0.4527 -0.5233 -0.6547 -0.8797 -1.1001
6 24 1 108 0 0 0 1.097E-19 0.000E+00
-0.0535 -0.0212 0.0629 0.1664 0.3603 0.4767 0.5737 0.6510
-0.1961 -0.2339 -0.3417 -0.4333 -0.5833 -0.7017 -0.8273 -0.9416
7 24 1 111 0 0 0 9.504E-19 0.000E+00
-0.0730 -0.0472 0.0692 0.2309 0.3860 0.7223 0.8257 0.8775 0.9098 0.9615
0.9784
0.8357 0.7948 0.5040 0.0594 -0.3997 -1.4577 -1.8085 -2.0036 -2.1385 -2.3877
-2.4726
8 24 1 112 0 0 0 1.046E-20 0.000E+00
-0.0756 -0.0562 -0.0045 0.1184 0.2865 0.4158 0.5257 0.6292 0.7068 0.7650
0.8296 0.9133
-1.0870 -1.1203 -1.2676 -1.6480 -2.2030 -2.6592 -3.0801 -3.4950 -3.7895 -3.9871
-4.1524 -4.3274
9 24 1 107 0 0 0 8.397E-20 0.000E+00
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-0.3428 -0.3700 -0.4535 -0.5863 -0.8056 -1.2490 -1.3478
10 24 1 110 0 0 0 1.690E-19 0.000E+00
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11 24 1 110 0 0 0 1.336E-18 0.000E+00
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12 24 1 109 0 0 0 3.240E-20 0.000E+00
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13 24 1 2 0 0 0 1.318E-18 0.000E+00
3.000 4.392 1.000 0.000
14 24 1 112 0 0 0 9.524E-20 0.000E+00
-0.1249 -0.1055 -0.0991 -0.0797 -0.0732 -0.0473 0.0302 0.1272 0.2630 0.4635
0.7350 0.9459
0.6998 0.3633 0.2451 -0.1366 -0.2501 -0.2882 -0.3439 -0.4320 -0.5859 -0.8523
-1.2525 -1.5748
15 24 1 114 0 0 0 2.605E-19 0.000E+00
-0.1249 -0.1055 -0.0861 -0.0797 -0.0473 0.0367 0.1337 0.2178 0.3018 0.4053
0.6057 0.7932 0.9549 0.9910
1.0398 0.7068 0.3846 0.3349 0.2321 0.0238 -0.1997 -0.3715 -0.5164 -0.6665
-0.9083 -1.1394 -1.3714 -1.4278
16 24 1 110 0 0 0 1.721E-18 0.000E+00
-0.1249 -0.1055 -0.0667 -0.0603 0.1596 0.3471 0.5152 0.6833 1.0583 1.1243
1.9833 1.6625 1.0928 1.0676 0.5832 0.1316 -0.3018 -0.7675 -1.8793 -2.0897
17 24 1 111 0 0 0 6.808E-20 0.000E+00
-0.1249 -0.1055 -0.0732 -0.0667 0.1531 0.3406 0.5217 0.6704 0.7803 0.8450
0.8939
0.6123 0.2874 -0.1899 -0.2770 -0.9059 -1.4927 -2.0898 -2.6085 -3.0203 -3.2845
-3.4928
18 24 1 2 0 0 0 1.581E-18 0.000E+00
3.000 5.270 1.000 0.000
19 24 1 2 0 0 0 1.581E-18 0.000E+00
3.000 5.271 1.000 0.000
20 24 1 105 0 0 0 9.665E-20 0.000E+00
0.002 0.276 0.649 0.916 1.311
-0.497 -1.210 -2.125 -2.715 -3.481
21 24 1 105 0 0 0 1.023E-19 0.000E+00
0.002 0.286 0.664 0.988 1.368
-0.472 -1.218 -2.162 -2.908 -3.669
22 24 1 105 0 0 0 1.110E-19 0.000E+00
0.002 0.276 0.667 1.066 1.468
-0.437 -1.169 -2.162 -3.099 -3.916
23 24 1 105 0 0 0 1.146E-19 0.000E+00
0.002 0.290 0.593 1.059 1.482
-0.423 -1.206 -1.989 -3.107 -4.005
*** Line transitions
1 2 -1 1 1 0 0 2.770E-01 7.000E-01
T 3 19 350. 0.
5.4E+8 1.9E-6 0. 0. 0.
1 3 -1 1 1 0 0 5.570E-01 7.000E-01
T 3 19 350. 0.
5.4E+8 1.9E-6 0. 0. 0.
1 4 0 0 4 0 0 0.000E+00 5.000E-02
1 5 0 0 4 0 0 0.000E+00 5.000E-02
1 6 -1 0 1 0 0 1.375E-02 2.000E-01
F 1 7 0. 0.
1 7 0 0 4 0 0 0.000E+00 5.000E-02
1 8 0 0 4 0 0 0.000E+00 5.000E-02
1 9 0 0 4 0 0 0.000E+00 5.000E-02
1 10 -1 0 1 0 0 7.950E-03 2.000E-01
F 1 7 0. 0.
1 11 0 0 4 0 0 0.000E+00 5.000E-02
1 12 0 0 4 0 0 0.000E+00 5.000E-02
1 13 0 0 4 0 0 0.000E+00 5.000E-02
1 14 0 0 4 0 0 0.000E+00 5.000E-02
1 15 -1 0 1 0 0 4.400E-03 2.000E-01
F 1 7 0. 0.
1 16 0 0 4 0 0 0.000E+00 5.000E-02
1 17 0 0 4 0 0 0.000E+00 5.000E-02
1 18 0 0 4 0 0 0.000E+00 5.000E-02
1 19 0 0 4 0 0 0.000E+00 5.000E-02
1 20 -1 0 1 0 0 2.645E-03 2.000E-01
F 1 7 0. 0.
1 21 -1 0 1 0 0 1.705E-03 2.000E-01
F 1 7 0. 0.
1 22 -1 0 1 0 0 1.165E-03 2.000E-01
F 1 7 0. 0.
1 23 -1 0 1 0 0 8.300E-04 2.000E-01
F 1 7 0. 0.
2 3 0 0 4 0 0 0.000E+00 5.000E-02
2 4 -1 0 1 0 0 8.867E-01 2.000E-01
F 1 7 0. 0.
2 5 -1 0 1 0 0 1.332E-01 2.000E-01
F 1 7 0. 0.
2 6 0 0 4 0 0 0.000E+00 5.000E-02
2 7 -1 0 1 0 0 9.083E-04 2.000E-01
F 1 7 0. 0.
2 8 0 0 4 0 0 0.000E+00 5.000E-02
2 9 -1 0 1 0 0 1.867E-02 2.000E-01
F 1 7 0. 0.
2 10 0 0 4 0 0 0.000E+00 5.000E-02
2 11 -1 0 1 0 0 6.717E-04 2.000E-01
F 1 7 0. 0.
2 12 0 0 4 0 0 0.000E+00 5.000E-02
2 13 0 0 4 0 0 0.000E+00 5.000E-02
2 14 -1 0 1 0 0 6.683E-03 2.000E-01
F 1 7 0. 0.
2 15 0 0 4 0 0 0.000E+00 5.000E-02
2 16 -1 0 1 0 0 9.567E-04 2.000E-01
F 1 7 0. 0.
2 17 0 0 4 0 0 0.000E+00 5.000E-02
2 18 0 0 4 0 0 0.000E+00 5.000E-02
2 19 0 0 4 0 0 0.000E+00 5.000E-02
2 20 -1 0 1 0 0 4.082E-03 2.000E-01
F 1 7 0. 0.
2 21 -1 0 1 0 0 2.498E-03 2.000E-01
F 1 7 0. 0.
2 22 -1 0 1 0 0 1.663E-03 2.000E-01
F 1 7 0. 0.
2 23 -1 0 1 0 0 1.168E-03 2.000E-01
F 1 7 0. 0.
3 4 -1 0 1 0 0 8.867E-01 2.000E-01
F 1 7 0. 0.
3 5 -1 0 1 0 0 1.332E-01 2.000E-01
F 1 7 0. 0.
3 6 0 0 4 0 0 0.000E+00 5.000E-02
3 7 -1 0 1 0 0 9.083E-04 2.000E-01
F 1 7 0. 0.
3 8 0 0 4 0 0 0.000E+00 5.000E-02
3 9 -1 0 1 0 0 1.867E-02 2.000E-01
F 1 7 0. 0.
3 10 0 0 4 0 0 0.000E+00 5.000E-02
3 11 -1 0 1 0 0 6.717E-04 2.000E-01
F 1 7 0. 0.
3 12 0 0 4 0 0 0.000E+00 5.000E-02
3 13 0 0 4 0 0 0.000E+00 5.000E-02
3 14 -1 0 1 0 0 6.683E-03 2.000E-01
F 1 7 0. 0.
3 15 0 0 4 0 0 0.000E+00 5.000E-02
3 16 -1 0 1 0 0 9.567E-04 2.000E-01
F 1 7 0. 0.
3 17 0 0 4 0 0 0.000E+00 5.000E-02
3 18 0 0 4 0 0 0.000E+00 5.000E-02
3 19 0 0 4 0 0 0.000E+00 5.000E-02
3 20 -1 0 1 0 0 4.082E-03 2.000E-01
F 1 7 0. 0.
3 21 -1 0 1 0 0 2.498E-03 2.000E-01
F 1 7 0. 0.
3 22 -1 0 1 0 0 1.663E-03 2.000E-01
F 1 7 0. 0.
3 23 -1 0 1 0 0 1.168E-03 2.000E-01
F 1 7 0. 0.
4 5 0 0 4 0 0 0.000E+00 5.000E-02
4 6 -1 0 1 0 0 1.660E-01 7.000E-01
F 1 7 0. 0.
4 7 0 0 4 0 0 0.000E+00 5.000E-02
4 8 -1 0 1 0 0 9.250E-01 2.000E-01
F 1 7 0. 0.
4 9 0 0 4 0 0 0.000E+00 5.000E-02
4 10 -1 0 1 0 0 1.060E-02 2.000E-01
F 1 7 0. 0.
4 11 0 0 4 0 0 0.000E+00 5.000E-02
4 12 -1 0 1 0 0 1.660E-01 2.000E-01
F 1 7 0. 0.
4 13 0 0 4 0 0 0.000E+00 5.000E-02
4 14 0 0 4 0 0 0.000E+00 5.000E-02
4 15 -1 0 1 0 0 3.270E-03 2.000E-01
F 1 7 0. 0.
4 16 0 0 4 0 0 0.000E+00 5.000E-02
4 17 -1 0 1 0 0 6.090E-02 2.000E-01
F 1 7 0. 0.
4 18 0 0 4 0 0 0.000E+00 5.000E-02
4 19 0 0 4 0 0 0.000E+00 5.000E-02
4 20 -1 0 1 0 0 3.141E-02 2.000E-01
F 1 7 0. 0.
4 21 -1 0 1 0 0 1.804E-02 2.000E-01
F 1 7 0. 0.
4 22 -1 0 1 0 0 1.142E-02 2.000E-01
F 1 7 0. 0.
4 23 -1 0 1 0 0 7.738E-03 2.000E-01
F 1 7 0. 0.
5 6 -1 0 1 0 0 1.290E+00 7.000E-01
F 1 7 0. 0.
5 7 0 0 4 0 0 0.000E+00 5.000E-02
5 8 0 0 4 0 0 0.000E+00 5.000E-02
5 9 0 0 4 0 0 0.000E+00 5.000E-02
5 10 -1 0 1 0 0 5.200E-03 2.000E-01
F 1 7 0. 0.
5 11 0 0 4 0 0 0.000E+00 5.000E-02
5 12 0 0 4 0 0 0.000E+00 5.000E-02
5 13 0 0 4 0 0 0.000E+00 5.000E-02
5 14 0 0 4 0 0 0.000E+00 5.000E-02
5 15 -1 0 1 0 0 5.000E-03 2.000E-01
F 1 7 0. 0.
5 16 0 0 4 0 0 0.000E+00 5.000E-02
5 17 0 0 4 0 0 0.000E+00 5.000E-02
5 18 0 0 4 0 0 0.000E+00 5.000E-02
5 19 0 0 4 0 0 0.000E+00 5.000E-02
5 20 -1 0 1 0 0 3.210E-03 2.000E-01
F 1 7 0. 0.
5 21 -1 0 1 0 0 2.090E-03 2.000E-01
F 1 7 0. 0.
5 22 -1 0 1 0 0 1.425E-03 2.000E-01
F 1 7 0. 0.
5 23 -1 0 1 0 0 1.010E-03 2.000E-01
F 1 7 0. 0.
6 7 -1 0 1 0 0 1.270E+00 2.000E-01
F 1 7 0. 0.
6 8 0 0 4 0 0 0.000E+00 5.000E-02
6 9 -1 0 1 0 0 2.350E-01 2.000E-01
F 1 7 0. 0.
6 10 0 0 4 0 0 0.000E+00 5.000E-02
6 11 -1 0 1 0 0 1.655E-02 2.000E-01
F 1 7 0. 0.
6 12 0 0 4 0 0 0.000E+00 5.000E-02
6 13 0 0 4 0 0 0.000E+00 5.000E-02
6 14 -1 0 1 0 0 3.183E-02 2.000E-01
F 1 7 0. 0.
6 15 0 0 4 0 0 0.000E+00 5.000E-02
6 16 -1 0 1 0 0 1.053E-03 2.000E-01
F 1 7 0. 0.
6 17 0 0 4 0 0 0.000E+00 5.000E-02
6 18 0 0 4 0 0 0.000E+00 5.000E-02
6 19 0 0 4 0 0 0.000E+00 5.000E-02
6 20 -1 0 1 0 0 1.138E-02 2.000E-01
F 1 7 0. 0.
6 21 -1 0 1 0 0 5.567E-03 2.000E-01
F 1 7 0. 0.
6 22 -1 0 1 0 0 3.228E-03 2.000E-01
F 1 7 0. 0.
6 23 -1 0 1 0 0 2.071E-03 2.000E-01
F 1 7 0. 0.
7 8 -1 0 1 0 0 1.060E-01 7.000E-01
F 1 7 0. 0.
7 9 0 0 4 0 0 0.000E+00 5.000E-02
7 10 -1 0 1 0 0 3.390E-01 7.000E-01
F 1 7 0. 0.
7 11 0 0 4 0 0 0.000E+00 5.000E-02
7 12 -1 0 1 0 0 7.280E-01 2.000E-01
F 1 7 0. 0.
7 13 0 0 4 0 0 0.000E+00 5.000E-02
7 14 0 0 4 0 0 0.000E+00 5.000E-02
7 15 -1 0 1 0 0 2.200E-02 2.000E-01
F 1 7 0. 0.
7 16 0 0 4 0 0 0.000E+00 5.000E-02
7 17 -1 0 1 0 0 1.790E-01 2.000E-01
F 1 7 0. 0.
7 18 0 0 4 0 0 0.000E+00 5.000E-02
7 19 0 0 4 0 0 0.000E+00 5.000E-02
7 20 -1 0 1 0 0 8.110E-02 2.000E-01
F 1 7 0. 0.
7 21 -1 0 1 0 0 4.215E-02 2.000E-01
F 1 7 0. 0.
7 22 -1 0 1 0 0 2.517E-02 2.000E-01
F 1 7 0. 0.
7 23 -1 0 1 0 0 1.641E-02 2.000E-01
F 1 7 0. 0.
8 9 0 0 4 0 0 0.000E+00 5.000E-02
8 10 0 0 4 0 0 0.000E+00 5.000E-02
8 11 -1 0 1 0 0 1.893E-02 2.000E-01
F 1 7 0. 0.
8 12 0 0 4 0 0 0.000E+00 5.000E-02
8 13 -1 0 1 0 0 1.344E+00 2.000E-01
F 1 7 0. 0.
8 14 0 0 4 0 0 0.000E+00 5.000E-02
8 15 0 0 4 0 0 0.000E+00 5.000E-02
8 16 -1 0 1 0 0 3.221E-03 2.000E-01
F 1 7 0. 0.
8 17 0 0 4 0 0 0.000E+00 5.000E-02
8 18 -1 0 1 0 0 2.117E-01 2.000E-01
F 1 7 0. 0.
8 19 0 0 4 0 0 0.000E+00 5.000E-02
8 20 -1 0 1 0 0 7.599E-02 2.000E-01
F 1 7 0. 0.
8 21 -1 0 1 0 0 3.686E-02 2.000E-01
F 1 7 0. 0.
8 22 -1 0 1 0 0 2.113E-02 2.000E-01
F 1 7 0. 0.
8 23 -1 0 1 0 0 1.343E-02 2.000E-01
F 1 7 0. 0.
9 10 -1 0 1 0 0 1.685E+00 7.000E-01
F 1 7 0. 0.
9 11 0 0 4 0 0 0.000E+00 5.000E-02
9 12 0 0 4 0 0 0.000E+00 5.000E-02
9 13 0 0 4 0 0 0.000E+00 5.000E-02
9 14 0 0 4 0 0 0.000E+00 5.000E-02
9 15 -1 0 1 0 0 2.045E-03 2.000E-01
F 1 7 0. 0.
9 16 0 0 4 0 0 0.000E+00 5.000E-02
9 17 0 0 4 0 0 0.000E+00 5.000E-02
9 18 0 0 4 0 0 0.000E+00 5.000E-02
9 19 0 0 4 0 0 0.000E+00 5.000E-02
9 20 -1 0 1 0 0 3.455E-03 2.000E-01
F 1 7 0. 0.
9 21 -1 0 1 0 0 2.500E-03 2.000E-01
F 1 7 0. 0.
9 22 -1 0 1 0 0 1.730E-03 2.000E-01
F 1 7 0. 0.
9 23 -1 0 1 0 0 1.230E-03 2.000E-01
F 1 7 0. 0.
10 11 -1 0 1 0 0 1.598E+00 2.000E-01
F 1 7 0. 0.
10 12 0 0 4 0 0 0.000E+00 5.000E-02
10 13 0 0 4 0 0 0.000E+00 5.000E-02
10 14 -1 0 1 0 0 3.383E-01 2.000E-01
F 1 7 0. 0.
10 15 0 0 4 0 0 0.000E+00 5.000E-02
10 16 -1 0 1 0 0 3.650E-02 2.000E-01
F 1 7 0. 0.
10 17 0 0 4 0 0 0.000E+00 5.000E-02
10 18 0 0 4 0 0 0.000E+00 5.000E-02
10 19 0 0 4 0 0 0.000E+00 5.000E-02
10 20 -1 0 1 0 0 4.973E-02 2.000E-01
F 1 7 0. 0.
10 21 -1 0 1 0 0 1.708E-02 2.000E-01
F 1 7 0. 0.
10 22 -1 0 1 0 0 8.225E-03 2.000E-01
F 1 7 0. 0.
10 23 -1 0 1 0 0 4.711E-03 2.000E-01
F 1 7 0. 0.
11 12 -1 0 1 0 0 1.960E-01 7.000E-01
F 1 7 0. 0.
11 13 0 0 4 0 0 0.000E+00 5.000E-02
11 14 0 0 4 0 0 0.000E+00 5.000E-02
11 15 -1 0 1 0 0 5.100E-01 7.000E-01
F 1 7 0. 0.
11 16 0 0 4 0 0 0.000E+00 5.000E-02
11 17 -1 0 1 0 0 6.430E-01 2.000E-01
F 1 7 0. 0.
11 18 0 0 4 0 0 0.000E+00 5.000E-02
11 19 0 0 4 0 0 0.000E+00 5.000E-02
11 20 -1 0 1 0 0 2.088E-01 2.000E-01
F 1 7 0. 0.
11 21 -1 0 1 0 0 8.730E-02 2.000E-01
F 1 7 0. 0.
11 22 -1 0 1 0 0 4.670E-02 2.000E-01
F 1 7 0. 0.
11 23 -1 0 1 0 0 2.845E-02 2.000E-01
F 1 7 0. 0.
12 13 -1 0 1 0 0 0.000E+00 7.000E-01
F 1 7 0. 0.
12 14 0 0 4 0 0 0.000E+00 5.000E-02
12 15 0 0 4 0 0 0.000E+00 5.000E-02
12 16 -1 0 1 0 0 4.679E-02 2.000E-01
F 1 7 0. 0.
12 17 0 0 4 0 0 0.000E+00 5.000E-02
12 18 -1 0 1 0 0 1.591E+00 2.000E-01
F 1 7 0. 0.
12 19 0 0 4 0 0 0.000E+00 5.000E-02
12 20 -1 0 1 0 0 2.515E-01 2.000E-01
F 1 7 0. 0.
12 21 -1 0 1 0 0 8.763E-02 2.000E-01
F 1 7 0. 0.
12 22 -1 0 1 0 0 4.217E-02 2.000E-01
F 1 7 0. 0.
12 23 -1 0 1 0 0 2.408E-02 2.000E-01
F 1 7 0. 0.
13 14 0 0 4 0 0 0.000E+00 5.000E-02
13 15 0 0 4 0 0 0.000E+00 5.000E-02
13 16 0 0 4 0 0 0.000E+00 5.000E-02
13 17 -1 0 1 0 0 1.591E+00 2.000E-01
F 1 7 0. 0.
13 18 0 0 4 0 0 0.000E+00 5.000E-02
13 19 -1 0 1 0 0 1.591E+00 2.000E-01
F 1 7 0. 0.
13 20 -1 0 1 0 0 4.864E-01 2.000E-01
F 1 7 0. 0.
13 21 -1 0 1 0 0 1.692E-01 2.000E-01
F 1 7 0. 0.
13 22 -1 0 1 0 0 8.137E-02 2.000E-01
F 1 7 0. 0.
13 23 -1 0 1 0 0 4.647E-02 2.000E-01
F 1 7 0. 0.
14 15 -1 0 1 0 0 2.070E+00 7.000E-01
F 1 7 0. 0.
14 16 0 0 4 0 0 0.000E+00 5.000E-02
14 17 0 0 4 0 0 0.000E+00 5.000E-02
14 18 0 0 4 0 0 0.000E+00 5.000E-02
14 19 0 0 4 0 0 0.000E+00 5.000E-02
14 20 -1 0 1 0 0 6.900E-04 2.000E-01
F 1 7 0. 0.
14 21 -1 0 1 0 0 2.520E-03 2.000E-01
F 1 7 0. 0.
14 22 -1 0 1 0 0 2.030E-03 2.000E-01
F 1 7 0. 0.
14 23 -1 0 1 0 0 1.480E-03 2.000E-01
F 1 7 0. 0.
15 16 -1 0 1 0 0 1.900E+00 2.000E-01
F 1 7 0. 0.
15 17 0 0 4 0 0 0.000E+00 5.000E-02
15 18 0 0 4 0 0 0.000E+00 5.000E-02
15 19 0 0 4 0 0 0.000E+00 5.000E-02
15 20 -1 0 1 0 0 4.953E-01 2.000E-01
F 1 7 0. 0.
15 21 -1 0 1 0 0 6.692E-02 2.000E-01
F 1 7 0. 0.
15 22 -1 0 1 0 0 2.317E-02 2.000E-01
F 1 7 0. 0.
15 23 -1 0 1 0 0 1.121E-02 2.000E-01
F 1 7 0. 0.
16 17 -1 0 1 0 0 2.750E-01 7.000E-01
F 1 7 0. 0.
16 18 0 0 4 0 0 0.000E+00 5.000E-02
16 19 0 0 4 0 0 0.000E+00 5.000E-02
16 20 -1 0 1 0 0 1.284E+00 2.000E-01
F 1 7 0. 0.
16 21 -1 0 1 0 0 2.160E-01 2.000E-01
F 1 7 0. 0.
16 22 -1 0 1 0 0 9.150E-02 2.000E-01
F 1 7 0. 0.
16 23 -1 0 1 0 0 4.954E-02 2.000E-01
F 1 7 0. 0.
17 18 -1 0 1 0 0 0.000E+00 7.000E-01
F 1 7 0. 0.
17 19 0 0 4 0 0 0.000E+00 5.000E-02
17 20 -1 0 1 0 0 1.916E+00 2.000E-01
F 1 7 0. 0.
17 21 -1 0 1 0 0 2.890E-01 2.000E-01
F 1 7 0. 0.
17 22 -1 0 1 0 0 9.953E-02 2.000E-01
F 1 7 0. 0.
17 23 -1 0 1 0 0 4.756E-02 2.000E-01
F 1 7 0. 0.
18 19 -1 0 1 0 0 0.000E+00 7.000E-01
F 1 7 0. 0.
18 20 -1 0 1 0 0 3.673E+00 2.000E-01
F 1 7 0. 0.
18 21 -1 0 1 0 0 5.486E-01 2.000E-01
F 1 7 0. 0.
18 22 -1 0 1 0 0 1.882E-01 2.000E-01
F 1 7 0. 0.
18 23 -1 0 1 0 0 8.973E-02 2.000E-01
F 1 7 0. 0.
19 20 -1 0 1 0 0 3.673E+00 2.000E-01
F 1 7 0. 0.
19 21 -1 0 1 0 0 5.486E-01 2.000E-01
F 1 7 0. 0.
19 22 -1 0 1 0 0 1.882E-01 2.000E-01
F 1 7 0. 0.
19 23 -1 0 1 0 0 8.973E-02 2.000E-01
F 1 7 0. 0.
20 21 -1 0 1 0 0 3.302E+00 2.000E-01
F 1 7 0. 0.
20 22 -1 0 1 0 0 4.861E-01 2.000E-01
F 1 7 0. 0.
20 23 -1 0 1 0 0 1.668E-01 2.000E-01
F 1 7 0. 0.
21 22 -1 0 1 0 0 3.921E+00 2.000E-01
F 1 7 0. 0.
21 23 -1 0 1 0 0 5.674E-01 2.000E-01
F 1 7 0. 0.
22 23 -1 0 1 0 0 4.508E+00 2.000E-01
F 1 7 0. 0.
File diff suppressed because it is too large Load Diff
+592
View File
@@ -0,0 +1,592 @@
****** Levels
5.89433957E+15 6. 2 'C II 2Po 1' 0 0. 0
4.60547088E+15 12. 3 'C II 4Pe 1' 0 0. 0
3.64928902E+15 10. 3 'C II 2De 1' 0 0. 0
3.00290047E+15 2. 3 'C II 2Se 1' 0 0. -104
2.57847422E+15 6. 3 'C II 2Pe 1' 0 0. -104
2.40202488E+15 2. 3 'C II 2Se 2' 0 0. -104
1.94653729E+15 6. 4 'C II 2Po 2' 0 0. -104
1.63790846E+15 4. 4 'C II 4So 1' 0 0. -104
1.53229293E+15 10. 4 'C II 2De 2' 0 0. -104
1.38499690E+15 10. 4 'C II 2Do 1' 0 0. -104
1.18203271E+15 2. 4 'C II 2Se 3' 0 0. -104
1.02350238E+15 6. 5 'C II 2Po 3' 0 0. -104
8.88993470E+14 12. 5 'C II 4Po 1' 0 0. -104
8.55573122E+14 10. 5 'C II 2De 3' 0 0. -104
8.37049263E+14 6. 5 'C II 2Po 4' 0 0. -104
8.29966191E+14 14. 5 'C II 2Fo 1' 0 0. -104
6.98977473E+14 2. 5 'C II 2Se 4' 0 0. -104
5.53884922E+14 54. 6 'C II+2__ 1' 0 0. -104
4.06452586E+14 36. 7 'C II+4_e 2' 0 0. -104
3.81543588E+14 78. 7 'C II+2__ 3' 0 0. -104
2.75013719E+14 72. 8 'C II+2__ 4' 0 0. -104
2.15914784E+14 60. 9 'C II+2__ 5' 0 0. -104
****** Continuum transitions
1 23 1 126 0 0 0 9.222E-19 0.000E+00
-0.0098 0.0096 0.0354 0.0419 0.0678 0.0872 0.1195 0.1260 0.1389 0.1648
0.1971 0.2488 0.3393 0.3523 0.7079 0.9148 1.0700 1.0765 1.1217 1.1476
1.1541 1.2252 1.3998 1.6002 1.8201 1.9238
0.6626 0.6870 0.7322 0.7334 0.6513 0.6257 0.5981 0.5868 0.5527 0.5354
0.4656 0.3856 0.2377 0.2323 -0.4698 -0.9093 -1.2605 -1.2439 -0.3396 -0.1746
-0.1773 -0.3440 -0.7928 -1.3399 -1.9683 -2.2759
2 23 1 106 0 0 0 2.736E-18 0.000E+00
0.1182 0.1635 0.1829 0.2669 0.3833 1.0456
0.9779 0.9122 0.8574 0.6701 0.4081 -1.5771
3 23 1 143 0 0 0 4.028E-19 0.000E+00
-0.0161 -0.0032 0.0033 0.0098 0.0162 0.0227 0.0292 0.0356 0.0421 0.0486
0.0550 0.0680 0.0744 0.0809 0.0874 0.0938 0.1003 0.1068 0.1132 0.1197
0.1326 0.1391 0.1456 0.1520 0.1585 0.1844 0.1908 0.2038 0.2102 0.2167
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0.056 -1.810 -1.070 -1.458 -2.180 -5.014
*** Line transitions
1 2 0 0 4 0 0 0.000E+00 2.8
1 3 -1 1 1 0 0 1.278E-01 7.000E-01
T 3 33 2000. 0.
2.7E+8 3.0E-7 0. 0. 0.
1 4 -1 1 1 0 0 1.245E-01 2.000E-01
T 3 29 1000. 0.
2.1E+9 3.6E-7 0. 0. 0.
1 5 -1 1 1 0 0 5.100E-01 2.000E-01
T 3 19 250. 0.
4.0E+9 0. 0. 0. 0.
1 6 -1 1 1 0 0 1.302E-02 2.000E-01
T 3 19 250. 0.
0. 3.3E-6 0. 0. 0.
1 7 0 0 4 0 0 0.000E+00 5.000E-02
1 8 0 0 4 0 0 0.000E+00 5.000E-02
1 9 -1 1 1 0 0 3.350E-01 2.000E-01
T 3 19 300. 0.
0. 6.8E-4 0. 0. 0.
1 10 0 0 4 0 0 0.000E+00 5.000E-02
1 11 -1 0 1 0 0 6.117E-03 2.000E-01
F 1 7 0. 0.
1 12 0 0 4 0 0 0.000E+00 5.000E-02
1 13 0 0 4 0 0 0.000E+00 5.000E-02
1 14 -1 0 1 0 0 1.173E-01 2.000E-01
F 1 7 0. 0.
1 15 0 0 4 0 0 0.000E+00 5.000E-02
1 16 0 0 4 0 0 0.000E+00 5.000E-02
1 17 -1 0 1 0 0 2.333E-03 2.000E-01
F 1 7 0. 0.
1 18 -1 0 1 0 0 5.700E-02 2.000E-01
F 1 7 0. 0.
1 19 0 0 4 0 0 0.000E+00 5.000E-02
1 20 -1 0 1 0 0 5.412E-02 2.000E-01
F 1 7 0. 0.
1 21 -1 0 1 0 0 3.044E-02 2.000E-01
F 1 7 0. 0.
1 22 -1 0 1 0 0 3.657E-02 2.000E-01
F 1 7 0. 0.
2 3 0 0 4 0 0 0.000E+00 5.000E-02
2 4 0 0 4 0 0 0.000E+00 5.000E-02
2 5 0 0 4 0 0 0.000E+00 5.000E-02
2 6 0 0 4 0 0 0.000E+00 5.000E-02
2 7 0 0 4 0 0 0.000E+00 5.000E-02
2 8 -1 0 1 0 0 1.767E-01 2.000E-01
F 1 7 0. 0.
2 9 0 0 4 0 0 0.000E+00 5.000E-02
2 10 0 0 4 0 0 0.000E+00 5.000E-02
2 11 0 0 4 0 0 0.000E+00 5.000E-02
2 12 0 0 4 0 0 0.000E+00 5.000E-02
2 13 -1 0 1 0 0 1.350E-01 2.000E-01
F 1 7 0. 0.
2 14 0 0 4 0 0 0.000E+00 5.000E-02
2 15 0 0 4 0 0 0.000E+00 5.000E-02
2 16 0 0 4 0 0 0.000E+00 5.000E-02
2 17 0 0 4 0 0 0.000E+00 5.000E-02
2 18 0 0 4 0 0 0.000E+00 5.000E-02
2 19 0 0 4 0 0 0.000E+00 5.000E-02
2 20 0 0 4 0 0 0.000E+00 5.000E-02
2 21 0 0 4 0 0 0.000E+00 5.000E-02
2 22 0 0 4 0 0 0.000E+00 5.000E-02
3 4 0 0 4 0 0 0.000E+00 5.000E-02
3 5 0 0 4 0 0 0.000E+00 5.000E-02
3 6 0 0 4 0 0 0.000E+00 5.000E-02
3 7 -1 0 1 0 0 1.180E-02 2.000E-01
F 1 7 0. 0.
3 8 0 0 4 0 0 0.000E+00 5.000E-02
3 9 0 0 4 0 0 0.000E+00 5.000E-02
3 10 -1 0 1 0 0 1.270E-01 2.000E-01
F 1 7 0. 0.
3 11 0 0 4 0 0 0.000E+00 5.000E-02
3 12 -1 0 1 0 0 1.850E-02 2.000E-01
F 1 7 0. 0.
3 13 0 0 4 0 0 0.000E+00 5.000E-02
3 14 0 0 4 0 0 0.000E+00 5.000E-02
3 15 -1 0 1 0 0 1.680E-01 2.000E-01
F 1 7 0. 0.
3 16 -1 0 1 0 0 3.670E-03 2.000E-01
F 1 7 0. 0.
3 17 0 0 4 0 0 0.000E+00 5.000E-02
3 18 -1 0 1 0 0 1.347E-02 2.000E-01
F 1 7 0. 0.
3 19 0 0 4 0 0 0.000E+00 5.000E-02
3 20 -1 0 1 0 0 1.639E-03 2.000E-01
F 1 7 0. 0.
3 21 -1 0 1 0 0 1.126E-03 2.000E-01
F 1 7 0. 0.
3 22 -1 0 1 0 0 8.116E-04 2.000E-01
F 1 7 0. 0.
4 5 0 0 4 0 0 0.000E+00 5.000E-02
4 6 0 0 4 0 0 0.000E+00 5.000E-02
4 7 -1 0 1 0 0 1.360E-01 2.000E-01
F 1 7 0. 0.
4 8 0 0 4 0 0 0.000E+00 5.000E-02
4 9 0 0 4 0 0 0.000E+00 5.000E-02
4 10 0 0 4 0 0 0.000E+00 5.000E-02
4 11 0 0 4 0 0 0.000E+00 5.000E-02
4 12 -1 0 1 0 0 4.860E-04 2.000E-01
F 1 7 0. 0.
4 13 0 0 4 0 0 0.000E+00 5.000E-02
4 14 0 0 4 0 0 0.000E+00 5.000E-02
4 15 -1 0 1 0 0 9.250E-04 2.000E-01
F 1 7 0. 0.
4 16 0 0 4 0 0 0.000E+00 5.000E-02
4 17 0 0 4 0 0 0.000E+00 5.000E-02
4 18 -1 0 1 0 0 1.480E-01 2.000E-01
F 1 7 0. 0.
4 19 0 0 4 0 0 0.000E+00 5.000E-02
4 20 -1 0 1 0 0 4.440E-03 2.000E-01
F 1 7 0. 0.
4 21 -1 0 1 0 0 5.550E-04 2.000E-01
F 1 7 0. 0.
4 22 -1 0 1 0 0 1.260E-04 2.000E-01
F 1 7 0. 0.
5 6 0 0 4 0 0 0.000E+00 5.000E-02
5 7 -1 0 1 0 0 2.133E-04 7.000E-01
F 1 7 0. 0.
5 8 0 0 4 0 0 0.000E+00 5.000E-02
5 9 0 0 4 0 0 0.000E+00 5.000E-02
5 10 -1 0 1 0 0 8.383E-02 2.000E-01
F 1 7 0. 0.
5 11 0 0 4 0 0 0.000E+00 5.000E-02
5 12 -1 0 1 0 0 6.233E-03 2.000E-01
F 1 7 0. 0.
5 13 0 0 4 0 0 0.000E+00 5.000E-02
5 14 0 0 4 0 0 0.000E+00 5.000E-02
5 15 -1 0 1 0 0 1.453E-01 2.000E-01
F 1 7 0. 0.
5 16 0 0 4 0 0 0.000E+00 5.000E-02
5 17 0 0 4 0 0 0.000E+00 5.000E-02
5 18 -1 0 1 0 0 3.108E-02 2.000E-01
F 1 7 0. 0.
5 19 0 0 4 0 0 0.000E+00 5.000E-02
5 20 -1 0 1 0 0 2.950E-06 2.000E-01
F 1 7 0. 0.
5 21 -1 0 1 0 0 3.650E-05 2.000E-01
F 1 7 0. 0.
5 22 -1 0 1 0 0 2.883E-05 2.000E-01
F 1 7 0. 0.
6 7 -1 0 1 0 0 6.900E-01 7.000E-01
F 1 7 0. 0.
6 8 0 0 4 0 0 0.000E+00 5.000E-02
6 9 0 0 4 0 0 0.000E+00 5.000E-02
6 10 0 0 4 0 0 0.000E+00 5.000E-02
6 11 0 0 4 0 0 0.000E+00 5.000E-02
6 12 -1 0 1 0 0 4.855E-02 2.000E-01
F 1 7 0. 0.
6 13 0 0 4 0 0 0.000E+00 5.000E-02
6 14 0 0 4 0 0 0.000E+00 5.000E-02
6 15 -1 0 1 0 0 6.500E-03 2.000E-01
F 1 7 0. 0.
6 16 0 0 4 0 0 0.000E+00 5.000E-02
6 17 0 0 4 0 0 0.000E+00 5.000E-02
6 18 -1 0 1 0 0 1.331E-02 2.000E-01
F 1 7 0. 0.
6 19 0 0 4 0 0 0.000E+00 5.000E-02
6 20 -1 0 1 0 0 8.600E-03 2.000E-01
F 1 7 0. 0.
6 21 -1 0 1 0 0 5.850E-03 2.000E-01
F 1 7 0. 0.
6 22 -1 0 1 0 0 3.945E-03 2.000E-01
F 1 7 0. 0.
7 8 0 0 4 0 0 0.000E+00 5.000E-02
7 9 -1 0 1 0 0 5.533E-01 7.000E-01
F 1 7 0. 0.
7 10 0 0 4 0 0 0.000E+00 5.000E-02
7 11 -1 0 1 0 0 1.458E-01 2.000E-01
F 1 7 0. 0.
7 12 0 0 4 0 0 0.000E+00 5.000E-02
7 13 0 0 4 0 0 0.000E+00 5.000E-02
7 14 -1 0 1 0 0 9.833E-02 2.000E-01
F 1 7 0. 0.
7 15 0 0 4 0 0 0.000E+00 5.000E-02
7 16 0 0 4 0 0 0.000E+00 5.000E-02
7 17 -1 0 1 0 0 2.217E-02 2.000E-01
F 1 7 0. 0.
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F 1 7 0. 0.
7 19 0 0 4 0 0 0.000E+00 5.000E-02
7 20 -1 0 1 0 0 4.987E-02 2.000E-01
F 1 7 0. 0.
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F 1 7 0. 0.
7 22 -1 0 1 0 0 3.269E-02 2.000E-01
F 1 7 0. 0.
8 9 0 0 4 0 0 0.000E+00 5.000E-02
8 10 0 0 4 0 0 0.000E+00 5.000E-02
8 11 0 0 4 0 0 0.000E+00 5.000E-02
8 12 0 0 4 0 0 0.000E+00 5.000E-02
8 13 0 0 4 0 0 0.000E+00 5.000E-02
8 14 0 0 4 0 0 0.000E+00 5.000E-02
8 15 0 0 4 0 0 0.000E+00 5.000E-02
8 16 0 0 4 0 0 0.000E+00 5.000E-02
8 17 0 0 4 0 0 0.000E+00 5.000E-02
8 18 0 0 4 0 0 0.000E+00 5.000E-02
8 19 -1 0 1 0 0 6.454E-02 2.000E-01
F 1 7 0. 0.
8 20 0 0 4 0 0 0.000E+00 5.000E-02
8 21 0 0 4 0 0 0.000E+00 5.000E-02
8 22 0 0 4 0 0 0.000E+00 5.000E-02
9 10 -1 0 1 0 0 5.450E-06 7.000E-01
F 1 7 0. 0.
9 11 0 0 4 0 0 0.000E+00 5.000E-02
9 12 -1 0 1 0 0 1.090E-01 2.000E-01
F 1 7 0. 0.
9 13 0 0 4 0 0 0.000E+00 5.000E-02
9 14 0 0 4 0 0 0.000E+00 5.000E-02
9 15 -1 0 1 0 0 2.210E-04 2.000E-01
F 1 7 0. 0.
9 16 -1 0 1 0 0 9.050E-01 2.000E-01
F 1 7 0. 0.
9 17 0 0 4 0 0 0.000E+00 5.000E-02
9 18 -1 0 1 0 0 1.627E-01 2.000E-01
F 1 7 0. 0.
9 19 0 0 4 0 0 0.000E+00 5.000E-02
9 20 -1 0 1 0 0 5.565E-02 2.000E-01
F 1 7 0. 0.
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F 1 7 0. 0.
9 22 -1 0 1 0 0 1.488E-02 2.000E-01
F 1 7 0. 0.
10 11 0 0 4 0 0 0.000E+00 5.000E-02
10 12 0 0 4 0 0 0.000E+00 5.000E-02
10 13 0 0 4 0 0 0.000E+00 5.000E-02
10 14 -1 0 1 0 0 2.700E-09 2.000E-01
F 1 7 0. 0.
10 15 0 0 4 0 0 0.000E+00 5.000E-02
10 16 0 0 4 0 0 0.000E+00 5.000E-02
10 17 0 0 4 0 0 0.000E+00 5.000E-02
10 18 -1 0 1 0 0 8.610E-06 2.000E-01
F 1 7 0. 0.
10 19 0 0 4 0 0 0.000E+00 5.000E-02
10 20 -1 0 1 0 0 2.095E-02 2.000E-01
F 1 7 0. 0.
10 21 -1 0 1 0 0 3.900E-04 2.000E-01
F 1 7 0. 0.
10 22 -1 0 1 0 0 6.940E-03 2.000E-01
F 1 7 0. 0.
11 12 -1 0 1 0 0 1.120E+00 7.000E-01
F 1 7 0. 0.
11 13 0 0 4 0 0 0.000E+00 5.000E-02
11 14 0 0 4 0 0 0.000E+00 5.000E-02
11 15 -1 0 1 0 0 1.555E-01 2.000E-01
F 1 7 0. 0.
11 16 0 0 4 0 0 0.000E+00 5.000E-02
11 17 0 0 4 0 0 0.000E+00 5.000E-02
11 18 -1 0 1 0 0 5.065E-02 2.000E-01
F 1 7 0. 0.
11 19 0 0 4 0 0 0.000E+00 5.000E-02
11 20 -1 0 1 0 0 2.700E-03 2.000E-01
F 1 7 0. 0.
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F 1 7 0. 0.
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F 1 7 0. 0.
12 13 0 0 4 0 0 0.000E+00 5.000E-02
12 14 -1 0 1 0 0 9.133E-01 7.000E-01
F 1 7 0. 0.
12 15 0 0 4 0 0 0.000E+00 5.000E-02
12 16 0 0 4 0 0 0.000E+00 5.000E-02
12 17 -1 0 1 0 0 1.967E-01 2.000E-01
F 1 7 0. 0.
12 18 -1 0 1 0 0 3.417E-02 2.000E-01
F 1 7 0. 0.
12 19 0 0 4 0 0 0.000E+00 5.000E-02
12 20 -1 0 1 0 0 7.767E-02 2.000E-01
F 1 7 0. 0.
12 21 -1 0 1 0 0 4.247E-02 2.000E-01
F 1 7 0. 0.
12 22 -1 0 1 0 0 8.317E-02 2.000E-01
F 1 7 0. 0.
13 14 0 0 4 0 0 0.000E+00 5.000E-02
13 15 0 0 4 0 0 0.000E+00 5.000E-02
13 16 0 0 4 0 0 0.000E+00 5.000E-02
13 17 0 0 4 0 0 0.000E+00 5.000E-02
13 18 0 0 4 0 0 0.000E+00 5.000E-02
13 19 -1 0 1 0 0 8.758E-01 2.000E-01
F 1 7 0. 0.
13 20 0 0 4 0 0 0.000E+00 5.000E-02
13 21 0 0 4 0 0 0.000E+00 5.000E-02
13 22 0 0 4 0 0 0.000E+00 5.000E-02
14 15 -1 0 1 0 0 2.580E-02 7.000E-01
F 1 7 0. 0.
14 16 -1 0 1 0 0 9.240E-02 7.000E-01
F 1 7 0. 0.
14 17 0 0 4 0 0 0.000E+00 5.000E-02
14 18 -1 0 1 0 0 9.182E-01 2.000E-01
F 1 7 0. 0.
14 19 0 0 4 0 0 0.000E+00 5.000E-02
14 20 -1 0 1 0 0 1.969E-01 2.000E-01
F 1 7 0. 0.
14 21 -1 0 1 0 0 7.974E-02 2.000E-01
F 1 7 0. 0.
14 22 -1 0 1 0 0 4.120E-02 2.000E-01
F 1 7 0. 0.
15 16 0 0 4 0 0 0.000E+00 5.000E-02
15 17 -1 0 1 0 0 4.983E-02 7.000E-01
F 1 7 0. 0.
15 18 -1 0 1 0 0 1.007E-01 2.000E-01
F 1 7 0. 0.
15 19 0 0 4 0 0 0.000E+00 5.000E-02
15 20 -1 0 1 0 0 7.972E-02 2.000E-01
F 1 7 0. 0.
15 21 -1 0 1 0 0 2.258E-03 2.000E-01
F 1 7 0. 0.
15 22 -1 0 1 0 0 2.704E-01 2.000E-01
F 1 7 0. 0.
16 17 0 0 4 0 0 0.000E+00 5.000E-02
16 18 -1 0 1 0 0 1.339E+00 2.000E-01
F 1 7 0. 0.
16 19 0 0 4 0 0 0.000E+00 5.000E-02
16 20 -1 0 1 0 0 1.895E-01 2.000E-01
F 1 7 0. 0.
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F 1 7 0. 0.
16 22 -1 0 1 0 0 2.817E-02 2.000E-01
F 1 7 0. 0.
17 18 -1 0 1 0 0 1.705E+00 2.000E-01
F 1 7 0. 0.
17 19 0 0 4 0 0 0.000E+00 5.000E-02
17 20 -1 0 1 0 0 6.700E-05 2.000E-01
F 1 7 0. 0.
17 21 -1 0 1 0 0 2.725E-03 2.000E-01
F 1 7 0. 0.
17 22 -1 0 1 0 0 2.650E-03 2.000E-01
F 1 7 0. 0.
18 19 0 0 4 0 0 0.000E+00 5.000E-02
18 20 -1 0 1 0 0 1.073E+00 2.000E-01
F 1 7 0. 0.
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F 1 7 0. 0.
18 22 -1 0 1 0 0 6.195E-02 2.000E-01
F 1 7 0. 0.
19 20 0 0 4 0 0 0.000E+00 5.000E-02
19 21 0 0 4 0 0 0.000E+00 5.000E-02
19 22 0 0 4 0 0 0.000E+00 5.000E-02
20 21 -1 0 1 0 0 1.317E+00 2.000E-01
F 1 7 0. 0.
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F 1 7 0. 0.
21 22 -1 0 1 0 0 1.073E+00 2.000E-01
F 1 7 0. 0.
File diff suppressed because it is too large Load Diff
+564
View File
@@ -0,0 +1,564 @@
****** Levels
1.55945583E+16 2. 2 'C IV 2Se 1' 0 0. 0
1.36613760E+16 2. 2 'C IV 2Po 1' 0 0. 0
1.36581470E+16 4. 2 'C IV 2Po 1' 0 0. 0
6.51537202E+15 2. 3 'C IV 2Se 2' 0 0. -104
5.99906956E+15 6. 3 'C IV 2Po 2' 0 0. -104
5.85471942E+15 10. 3 'C IV 2De 1' 0 0. -104
3.56244314E+15 2. 4 'C IV 2Se 3' 0 0. -104
3.35343089E+15 6. 4 'C IV 2Po 3' 0 0. -104
3.29290270E+15 10. 4 'C IV 2De 2' 0 0. -104
3.29005464E+15 14. 4 'C IV 2Fo 1' 0 0. -104
2.24274451E+15 2. 5 'C IV 2Se 4' 0 0. -104
2.13804208E+15 6. 5 'C IV 2Po 4' 0 0. -104
2.10722340E+15 10. 5 'C IV 2De 3' 0 0. -104
2.10569456E+15 14. 5 'C IV 2Fo 2' 0 0. -104
2.10534700E+15 18. 5 'C IV 2Ge 1' 0 0. -104
1.54076546E+15 2. 6 'C IV 2Se 5' 0 0. -104
1.48098690E+15 6. 6 'C IV 2Po 5' 0 0. -104
1.46320923E+15 10. 6 'C IV 2De 4' 0 0. -104
1.46217612E+15 14. 6 'C IV 2Fo 3' 0 0. -104
1.46207116E+15 18. 6 'C IV 2Ge 2' 0 0. -104
1.46207116E+15 22. 6 'C IV 2Ho 1' 0 0. -104
1.07611553E+15 98. 7 'C IV+2__ 1' 0 0. -104
8.23387643E+14 128. 8 'C IV+2__ 2' 0 0. -104
6.50353008E+14 162. 9 'C IV+2__ 3' 0 0. -104
5.27233844E+14 200. 10 'C IV+2__ 4' 0 0. -104
****** Continuum transitions
1 26 1 116 0 0 0 1.922E-19 0.000E+00
-0.0149 0.0110 0.1338 0.2761 0.3795 0.5541 0.7093 0.7545 0.7610 0.7675
0.7739 0.7804 0.7998 0.9744 1.1619 1.3246
-0.1726 -0.2005 -0.4114 -0.6842 -0.8897 -1.2472 -1.5886 -0.5243 -0.4333 -0.3678
-0.3427 -0.3320 -0.3668 -0.8011 -1.2988 -1.7537
2 26 1 108 0 0 0 2.772E-19 0.000E+00
-0.0171 0.0023 0.0541 0.2674 0.4808 0.7007 0.8623 0.9282
-0.0092 -0.0412 -0.1868 -0.8370 -1.5232 -2.2674 -2.8414 -3.0814
3 26 1 108 0 0 0 2.772E-19 0.000E+00
-0.0171 0.0023 0.0541 0.2674 0.4808 0.7007 0.8623 0.9282
-0.0092 -0.0412 -0.1868 -0.8370 -1.5232 -2.2674 -2.8414 -3.0814
4 26 1 109 0 0 0 3.084E-19 0.000E+00
-0.0366 -0.0042 0.2027 0.4354 0.6747 0.9010 1.1273 1.3407 1.3992
0.0721 0.0351 -0.3305 -0.7769 -1.2693 -1.7703 -2.3024 -2.8347 -2.9876
5 26 1 109 0 0 0 5.091E-19 0.000E+00
-0.0399 -0.0140 0.1347 0.3158 0.4968 0.6779 0.8589 1.0012 1.0519
0.3084 0.2711 -0.0822 -0.5455 -1.0418 -1.5711 -2.1332 -2.6012 -2.7726
6 26 1 108 0 0 0 3.390E-19 0.000E+00
-0.0409 -0.0215 0.0173 0.1919 0.3665 0.5346 0.7092 0.7816
0.1638 0.1269 0.0021 -0.6157 -1.2675 -1.9286 -2.6505 -2.9646
7 26 1 108 0 0 0 4.609E-19 0.000E+00
-0.0694 -0.0371 0.2216 0.5125 0.8035 1.0880 1.3790 1.4598
0.2878 0.2494 -0.2184 -0.7788 -1.3730 -1.9865 -2.6479 -2.8398
8 26 1 109 0 0 0 7.655E-19 0.000E+00
-0.0741 -0.0483 0.1199 0.3268 0.5272 0.7212 0.9475 1.0962 1.1401
0.5495 0.5143 0.1480 -0.3350 -0.8361 -1.3552 -2.0028 -2.4543 -2.5902
9 26 1 109 0 0 0 6.781E-19 0.000E+00
-0.0756 -0.0497 0.0602 0.2154 0.3706 0.5258 0.6745 0.8232 0.9135
0.5357 0.4910 0.1880 -0.2720 -0.7644 -1.2901 -1.8260 -2.3938 -2.7587
10 26 1 2 0 0 0 5.928E-19 0.000E+00
3.000 1.976 1.000 0.000
11 26 1 107 0 0 0 6.079E-19 0.000E+00
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0.5010 0.4613 -0.0264 -0.7259 -1.4214 -2.1911 -2.7199
12 26 1 109 0 0 0 1.035E-18 0.000E+00
-0.1227 -0.0903 0.1554 0.3946 0.6145 0.8149 1.0024 1.1641 1.2124
0.7804 0.7343 0.2107 -0.3311 -0.8619 -1.3783 -1.8938 -2.3545 -2.4957
13 26 1 110 0 0 0 1.023E-18 0.000E+00
-0.1247 -0.0924 0.0693 0.2374 0.3991 0.5542 0.7094 0.8582 1.0069 1.0878
0.8125 0.7591 0.3574 -0.0919 -0.5565 -1.0343 -1.5452 -2.0673 -2.6230 -2.9442
14 26 1 2 0 0 0 7.412E-19 0.000E+00
3.000 2.471 1.000 0.000
15 26 1 2 0 0 0 7.413E-19 0.000E+00
3.000 2.471 1.000 0.000
16 26 1 107 0 0 0 7.872E-19 0.000E+00
-0.0997 -0.0544 0.3853 0.7991 1.1742 1.4910 1.5002
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1.2353
0.8832 0.8033 0.2903 -0.1780 -0.6451 -1.1263 -1.6206 -2.1264 -2.6658 -3.0660
-3.1263
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3.000 2.965 1.000 0.000
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3.000 2.965 1.000 0.000
21 26 1 2 0 0 0 8.895E-19 0.000E+00
3.000 2.965 1.000 0.000
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-0.537 -4.313
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25 26 1 104 0 0 0 6.948E-20 0.000E+00
0.003 0.505 1.075 1.662
-0.643 -2.042 -3.512 -4.877
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2.6E+8 7.9E-7 0. 0. 0.
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F 1 7 0. 0.
20 23 -1 0 1 0 0 5.486E-01 2.000E-01
F 1 7 0. 0.
20 24 -1 0 1 0 0 1.882E-01 2.000E-01
F 1 7 0. 0.
20 25 -1 0 1 0 0 8.973E-02 2.000E-01
F 1 7 0. 0.
21 22 -1 0 1 0 0 3.673E+00 2.000E-01
F 1 7 0. 0.
21 23 -1 0 1 0 0 5.486E-01 2.000E-01
F 1 7 0. 0.
21 24 -1 0 1 0 0 1.882E-01 2.000E-01
F 1 7 0. 0.
21 25 -1 0 1 0 0 8.973E-02 2.000E-01
F 1 7 0. 0.
22 23 -1 0 1 0 0 3.680E+00 2.000E-01
F 1 7 0. 0.
22 24 -1 0 1 0 0 5.466E-01 2.000E-01
F 1 7 0. 0.
22 25 -1 0 1 0 0 1.869E-01 2.000E-01
F 1 7 0. 0.
23 24 -1 0 1 0 0 4.240E+00 2.000E-01
F 1 7 0. 0.
23 25 -1 0 1 0 0 6.185E-01 2.000E-01
F 1 7 0. 0.
24 25 -1 0 1 0 0 4.783E+00 2.000E-01
F 1 7 0. 0.
File diff suppressed because it is too large Load Diff
+797
View File
@@ -0,0 +1,797 @@
****** Levels
3.90170048E+15 30. 2 ' even 1 ' 2 0. 0
3.84173383E+15 28. 2 ' even 2 ' 2 0. 0
3.66473941E+15 20. 2 ' even 3 ' 2 0. 0
3.44453390E+15 36. 2 ' even 4 ' 2 0. 0
3.26538876E+15 122. 2 ' even 5 ' 2 0. 0
3.12772061E+15 78. 2 ' even 6 ' 2 0. 0
2.95137693E+15 96. 2 ' even 7 ' 2 0. 0
2.79906051E+15 22. 2 ' even 8 ' 2 0. 0
2.75368871E+15 30. 2 ' odd 1 ' 2 0. 0
2.60013558E+15 120. 2 ' odd 2 ' 2 0. 0
2.56747507E+15 14. 2 ' even 9 ' 2 0. 0
2.42680383E+15 50. 2 ' even 10 ' 2 0. 0
2.33513048E+15 24. 2 ' odd 3 ' 2 0. 0
2.21660728E+15 106. 2 ' even 11 ' 2 0. 0
2.00156526E+15 552. 3 ' odd 4 ' 2 0. -110
1.76789433E+15 78. 3 ' even 12 ' 2 0. -110
1.70131844E+15 294. 3 ' odd 5 ' 2 0. -110
1.55490013E+15 114. 3 ' even 13 ' 2 0. -110
1.37400895E+15 252. 3 ' even 14 ' 2 0. -110
1.16684150E+15 984. 3 ' odd 6 ' 2 0. -110
9.56438295E+14 138. 4 ' even 15 ' 2 0. -110
7.42804055E+14 1456. 4 ' even 16 ' 2 0. -110
6.26560687E+14 2670. 5 ' odd 7 ' 2 0. -110
3.02043038E+14 4140. 7 ' even 17 ' 2 0. -110
2.13630326E+14 3240. 8 ' odd 8 ' 2 0. -110
-3.17856437E+14 13358. 20 ' even 18 ' 0 0. -110
-3.32682518E+14 9022. 20 ' odd 9 ' 0 0. -110
-8.33913111E+14 7470. 20 ' even 19 ' 0 0. -110
-1.15510396E+15 7586. 20 ' odd 10 ' 0 0. -110
-1.24668824E+15 8184. 20 ' even 20 ' 0 0. -110
-1.76743572E+15 6826. 20 ' even 21 ' 0 0. -110
-1.89398155E+15 11618. 20 ' odd 11 ' 0 0. -110
-2.37330132E+15 1848. 20 ' even 22 ' 0 0. -110
-2.73687754E+15 2838. 20 ' odd 12 ' 0 0. -110
-3.02487329E+15 1182. 20 ' even 23 ' 0 0. -110
-3.54043362E+15 838. 20 ' odd 13 ' 0 0. -110
****** Continuum transitions
1 37 1 61 0 0 0 7.26E-19 0.
2 37 1 61 0 0 0 7.32E-19 0.
3 37 1 61 0 0 0 7.49E-19 0.
4 37 1 61 0 0 0 7.73E-19 0.
5 37 1 61 0 0 0 7.94E-19 0.
6 37 1 61 0 0 0 8.11E-19 0.
7 37 1 61 0 0 0 8.35E-19 0.
8 37 1 61 0 0 0 8.57E-19 0.
9 37 1 61 0 0 0 8.64E-19 0.
10 37 1 61 0 0 0 8.89E-19 0.
11 37 1 61 0 0 0 8.95E-19 0.
12 37 1 61 0 0 0 9.21E-19 0.
13 37 1 61 0 0 0 9.38E-19 0.
14 37 1 61 0 0 0 9.63E-19 0.
15 37 1 61 0 0 0 1.01E-18 0.
16 37 1 61 0 0 0 1.08E-18 0.
17 37 1 61 0 0 0 1.10E-18 0.
18 37 1 61 0 0 0 1.15E-18 0.
19 37 1 61 0 0 0 1.22E-18 0.
20 37 1 61 0 0 0 1.33E-18 0.
21 37 1 61 0 0 0 1.47E-18 0.
22 37 1 61 0 0 0 1.66E-18 0.
23 37 1 61 0 0 0 1.81E-18 0.
24 37 1 61 0 0 0 2.61E-18 0.
25 37 1 61 0 0 0 3.10E-18 0.
26 37 0 0 0 0 0 1.00E-12 0.
27 37 0 0 0 0 0 1.00E-12 0.
28 37 0 0 0 0 0 1.00E-12 0.
29 37 0 0 0 0 0 1.00E-12 0.
30 37 0 0 0 0 0 1.00E-12 0.
31 37 0 0 0 0 0 1.00E-12 0.
32 37 0 0 0 0 0 1.00E-12 0.
33 37 0 0 0 0 0 1.00E-12 0.
34 37 0 0 0 0 0 1.00E-12 0.
35 37 0 0 0 0 0 1.00E-12 0.
36 37 0 0 0 0 0 1.00E-12 0.
*** Line transitions
1 2 0 0 9 0 0 0. 0.05
1 3 0 0 9 0 0 0. 0.05
1 4 0 0 9 0 0 0. 0.05
1 5 0 0 9 0 0 0. 0.05
1 6 0 0 9 0 0 0. 0.05
1 7 0 0 9 0 0 0. 0.05
1 8 0 0 9 0 0 0. 0.05
1 9 -3 0 9 0 0 0. 0.05
1 10 -3 0 9 0 0 0. 0.05
1 11 0 0 9 0 0 0. 0.05
1 12 0 0 9 0 0 0. 0.05
1 13 -3 0 9 0 0 0. 0.05
1 14 0 0 9 0 0 0. 0.05
1 15 -3 0 9 0 0 0. 0.05
1 16 0 0 9 0 0 0. 0.05
1 17 -3 0 9 0 0 0. 0.05
1 18 0 0 9 0 0 0. 0.05
1 19 0 0 9 0 0 0. 0.05
1 20 -3 0 9 0 0 0. 0.05
1 21 0 0 9 0 0 0. 0.05
1 22 0 0 9 0 0 0. 0.05
1 23 -3 0 9 0 0 0. 0.05
1 23 -3 0 9 0 0 0. 0.05
1 24 0 0 9 0 0 0. 0.05
1 25 -3 0 9 0 0 0. 0.05
1 26 0 0 9 0 0 0. 0.05
1 27 -3 0 9 0 0 0. 0.05
1 28 0 0 9 0 0 0. 0.05
1 29 -3 0 9 0 0 0. 0.05
1 30 0 0 9 0 0 0. 0.05
1 31 0 0 9 0 0 0. 0.05
1 32 -3 0 9 0 0 0. 0.05
1 33 0 0 9 0 0 0. 0.05
1 34 -3 0 9 0 0 0. 0.05
1 35 0 0 9 0 0 0. 0.05
1 36 -3 0 9 0 0 0. 0.05
2 3 0 0 9 0 0 0. 0.05
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2 5 0 0 9 0 0 0. 0.05
2 6 0 0 9 0 0 0. 0.05
2 7 0 0 9 0 0 0. 0.05
2 8 0 0 9 0 0 0. 0.05
2 9 -3 0 9 0 0 0. 0.05
2 10 -3 0 9 0 0 0. 0.05
2 11 0 0 9 0 0 0. 0.05
2 12 0 0 9 0 0 0. 0.05
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2 20 -3 0 9 0 0 0. 0.05
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2 23 -3 0 9 0 0 0. 0.05
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2 30 0 0 9 0 0 0. 0.05
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2 33 0 0 9 0 0 0. 0.05
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2 35 0 0 9 0 0 0. 0.05
2 36 -3 0 9 0 0 0. 0.05
3 4 0 0 9 0 0 0. 0.05
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3 6 0 0 9 0 0 0. 0.05
3 7 0 0 9 0 0 0. 0.05
3 8 0 0 9 0 0 0. 0.05
3 9 -3 0 9 0 0 0. 0.05
3 10 -3 0 9 0 0 0. 0.05
3 11 0 0 9 0 0 0. 0.05
3 12 0 0 9 0 0 0. 0.05
3 13 -3 0 9 0 0 0. 0.05
3 14 0 0 9 0 0 0. 0.05
3 15 -3 0 9 0 0 0. 0.05
3 16 0 0 9 0 0 0. 0.05
3 17 -3 0 9 0 0 0. 0.05
3 18 0 0 9 0 0 0. 0.05
3 19 0 0 9 0 0 0. 0.05
3 20 -3 0 9 0 0 0. 0.05
3 21 0 0 9 0 0 0. 0.05
3 22 0 0 9 0 0 0. 0.05
3 23 -3 0 9 0 0 0. 0.05
3 24 0 0 9 0 0 0. 0.05
3 25 -3 0 9 0 0 0. 0.05
3 25 -3 0 9 0 0 0. 0.05
3 26 0 0 9 0 0 0. 0.05
3 27 -3 0 9 0 0 0. 0.05
3 28 0 0 9 0 0 0. 0.05
3 29 -3 0 9 0 0 0. 0.05
3 30 0 0 9 0 0 0. 0.05
3 31 0 0 9 0 0 0. 0.05
3 32 -3 0 9 0 0 0. 0.05
3 33 0 0 9 0 0 0. 0.05
3 34 -3 0 9 0 0 0. 0.05
3 35 0 0 9 0 0 0. 0.05
3 36 -3 0 9 0 0 0. 0.05
4 5 0 0 9 0 0 0. 0.05
4 6 0 0 9 0 0 0. 0.05
4 7 0 0 9 0 0 0. 0.05
4 8 0 0 9 0 0 0. 0.05
4 9 -3 0 9 0 0 0. 0.05
4 10 -3 0 9 0 0 0. 0.05
4 10 -3 0 9 0 0 0. 0.05
4 11 0 0 9 0 0 0. 0.05
4 12 0 0 9 0 0 0. 0.05
4 13 -3 0 9 0 0 0. 0.05
4 14 0 0 9 0 0 0. 0.05
4 15 -3 0 9 0 0 0. 0.05
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4 17 -3 0 9 0 0 0. 0.05
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4 25 -3 0 9 0 0 0. 0.05
4 26 0 0 9 0 0 0. 0.05
4 27 -3 0 9 0 0 0. 0.05
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4 29 -3 0 9 0 0 0. 0.05
4 30 0 0 9 0 0 0. 0.05
4 31 0 0 9 0 0 0. 0.05
4 32 -3 0 9 0 0 0. 0.05
4 33 0 0 9 0 0 0. 0.05
4 34 -3 0 9 0 0 0. 0.05
4 35 0 0 9 0 0 0. 0.05
4 36 -3 0 9 0 0 0. 0.05
5 6 0 0 9 0 0 0. 0.05
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5 8 0 0 9 0 0 0. 0.05
5 9 -3 0 9 0 0 0. 0.05
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5 20 -3 0 9 0 0 0. 0.05
5 21 0 0 9 0 0 0. 0.05
5 22 0 0 9 0 0 0. 0.05
5 23 -3 0 9 0 0 0. 0.05
5 24 0 0 9 0 0 0. 0.05
5 25 -3 0 9 0 0 0. 0.05
5 25 -3 0 9 0 0 0. 0.05
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5 27 -3 0 9 0 0 0. 0.05
5 27 -3 0 9 0 0 0. 0.05
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5 30 0 0 9 0 0 0. 0.05
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22 25 -3 0 9 0 0 0. 0.05
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23 25 0 0 9 0 0 0. 0.05
23 26 -3 0 9 0 0 0. 0.05
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23 27 0 0 9 0 0 0. 0.05
23 28 -3 0 9 0 0 0. 0.05
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23 35 -3 0 9 0 0 0. 0.05
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24 27 -3 0 9 0 0 0. 0.05
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24 29 -3 0 9 0 0 0. 0.05
24 29 -3 0 9 0 0 0. 0.05
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25 26 -3 0 9 0 0 0. 0.05
25 26 -3 0 9 0 0 0. 0.05
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25 28 -3 0 9 0 0 0. 0.05
25 28 -3 0 9 0 0 0. 0.05
25 29 0 0 9 0 0 0. 0.05
25 30 -3 0 9 0 0 0. 0.05
25 31 -3 0 9 0 0 0. 0.05
25 32 0 0 9 0 0 0. 0.05
25 33 -3 0 9 0 0 0. 0.05
25 34 0 0 9 0 0 0. 0.05
25 35 -3 0 9 0 0 0. 0.05
25 35 -3 0 9 0 0 0. 0.05
25 36 0 0 9 0 0 0. 0.05
26 27 0 0 9 0 0 0. 0.05
26 28 0 0 9 0 0 0. 0.05
26 29 0 0 9 0 0 0. 0.05
26 30 0 0 9 0 0 0. 0.05
26 31 0 0 9 0 0 0. 0.05
26 32 0 0 9 0 0 0. 0.05
26 33 0 0 9 0 0 0. 0.05
26 34 0 0 9 0 0 0. 0.05
26 35 0 0 9 0 0 0. 0.05
26 36 0 0 9 0 0 0. 0.05
27 28 0 0 9 0 0 0. 0.05
27 29 0 0 9 0 0 0. 0.05
27 30 0 0 9 0 0 0. 0.05
27 31 0 0 9 0 0 0. 0.05
27 32 0 0 9 0 0 0. 0.05
27 33 0 0 9 0 0 0. 0.05
27 34 0 0 9 0 0 0. 0.05
27 35 0 0 9 0 0 0. 0.05
27 36 0 0 9 0 0 0. 0.05
28 29 0 0 9 0 0 0. 0.05
28 30 0 0 9 0 0 0. 0.05
28 31 0 0 9 0 0 0. 0.05
28 32 0 0 9 0 0 0. 0.05
28 33 0 0 9 0 0 0. 0.05
28 34 0 0 9 0 0 0. 0.05
28 35 0 0 9 0 0 0. 0.05
28 36 0 0 9 0 0 0. 0.05
29 30 0 0 9 0 0 0. 0.05
29 31 0 0 9 0 0 0. 0.05
29 32 0 0 9 0 0 0. 0.05
29 33 0 0 9 0 0 0. 0.05
29 34 0 0 9 0 0 0. 0.05
29 35 0 0 9 0 0 0. 0.05
29 36 0 0 9 0 0 0. 0.05
30 31 0 0 9 0 0 0. 0.05
30 32 0 0 9 0 0 0. 0.05
30 33 0 0 9 0 0 0. 0.05
30 34 0 0 9 0 0 0. 0.05
30 35 0 0 9 0 0 0. 0.05
30 36 0 0 9 0 0 0. 0.05
31 32 0 0 9 0 0 0. 0.05
31 33 0 0 9 0 0 0. 0.05
31 34 0 0 9 0 0 0. 0.05
31 35 0 0 9 0 0 0. 0.05
31 36 0 0 9 0 0 0. 0.05
32 33 0 0 9 0 0 0. 0.05
32 34 0 0 9 0 0 0. 0.05
32 35 0 0 9 0 0 0. 0.05
32 36 0 0 9 0 0 0. 0.05
33 34 0 0 9 0 0 0. 0.05
33 35 0 0 9 0 0 0. 0.05
33 36 0 0 9 0 0 0. 0.05
34 35 0 0 9 0 0 0. 0.05
34 36 0 0 9 0 0 0. 0.05
35 36 0 0 9 0 0 0. 0.05
****** Energy bands
23
1000.
5000.
10000.
20000.
25000.
30000.
35000.
40000.
45000.
52000.
65000.
75000.
82000.
90000.
101000.
112000.
131000.
150000.
165000.
180000.
200000.
220000.
250000.
13
40000.
50000.
55000.
70000.
80000.
100000.
116000.
131000.
155000.
180000.
210000.
240000.
280000.
File diff suppressed because it is too large Load Diff
File diff suppressed because it is too large Load Diff
File diff suppressed because it is too large Load Diff
File diff suppressed because it is too large Load Diff
File diff suppressed because it is too large Load Diff
File diff suppressed because it is too large Load Diff
+91
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@@ -0,0 +1,91 @@
****** Levels
0. 0. 0 ' (N=1) ' 1 0. 0
0. 0. 0 ' (N=2) ' 1 0. 0
0. 0. 0 ' (N=3) ' 1 0. 0
0. 0. 0 ' (N=4) ' 1 0. 0
0. 0. 0 ' (N=5) ' 1 0. -105
0. 0. 0 ' (N=6) ' 1 0. -105
0. 0. 0 ' (N=7) ' 1 0. -105
0. 0. 0 ' (N=8) ' 1 0. -105
0. 0. 0 ' (N=9) ' -1 0. -105
****** Continuum transitions
1 10 5 1 0 1 6 0. 0.
2.6D15
2 10 5 1 0 0 0 0. 0.
5.4D14
3 10 5 1 0 0 0 0. 0.
2.0D14
4 10 1 1 0 0 0 0. 0.
5 10 1 1 0 0 0 0. 0.
6 10 1 1 0 0 0 0. 0.
7 10 1 1 0 0 0 0. 0.
8 10 1 1 0 0 0 0. 0.
9 10 1 1 0 0 0 0. 0.
****** Line transitions
1 2 -1 2 0 26 28 0. 0. ! H I Lyman LINES ! 51
T 3 27 1022. 0.
1 3 -1 2 0 23 23 0. 0.
T 3 23 510. 0.
1 4 -1 2 0 23 23 0. 0.
T 3 23 510. 0.
1 5 -1 2 0 0 0 0. 0.
T 3 21 254. 0.
1 6 -1 2 0 0 0 0. 0.
T 3 21 254. 0.
1 7 -1 2 0 0 0 0. 0.
T 3 21 254. 0.
1 8 -1 2 0 0 0 0. 0.
T 3 21 254. 0.
1 9 -2 0 0 0 0 0. 0.
3 3 5 1.5 15. 15. 3
2 3 -1 2 0 17 17 0. 0. ! H-alpha ! 13
T 3 17 510. 0.
2 4 -1 2 0 17 17 0. 0.
T 3 17 510. 0.
2 5 -1 2 0 0 0 0. 0.
T 3 17 510. 0.
2 6 -1 2 0 0 0 0. 0.
T 3 15 254. 0.
2 7 -1 2 0 0 0 0. 0.
T 3 15 254. 0.
2 8 -1 2 0 0 0 0. 0.
T 3 15 254. 0.
2 9 -2 0 0 0 0 0. 0.
3 3 5 1.5 15. 15. 3
3 4 -1 2 0 0 0 0. 0.
T 3 15 254. 0.
3 5 -1 2 0 0 0 0. 0.
T 3 15 254. 0.
3 6 -1 2 0 0 0 0. 0.
T 3 13 126. 0.
3 7 -1 2 0 0 0 0. 0.
T 3 13 126. 0.
3 8 -1 2 0 0 0 0. 0.
T 3 13 126. 0.
3 9 -2 0 0 0 0 0. 0.
3 3 5 1.5 15. 15. 3
4 5 -1 0 0 0 0 0. 0.
F 1 7 0. 0.
4 6 -1 0 0 0 0 0. 0.
F 1 7 0. 0.
4 7 -1 0 0 0 0 0. 0.
F 1 7 0. 0.
4 8 -1 0 0 0 0 0. 0.
F 1 7 0. 0.
4 9 0 0 0 0 0 0. 0.
5 6 -1 0 0 0 0 0. 0.
F 1 7 0. 0.
5 7 -1 0 0 0 0 0. 0
F 1 7 0. 0.
5 8 -1 0 0 0 0 0. 0
F 1 7 0. 0.
5 9 0 0 0 0 0 0. 0
6 7 -1 0 0 0 0 0. 0. ! 49
F 1 7 0. 0.
6 8 -1 0 0 0 0 0. 0.
F 1 7 0. 0.
6 9 0 0 0 0 0 0. 0.
7 8 -1 0 0 0 0 0. 0. ! 49
F 1 7 0. 0.
7 9 0 0 0 0 0 0. 0.
8 9 0 0 0 0 0 0. 0. ! 49
+448
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@@ -0,0 +1,448 @@
****** Levels
5.94503520D+15 1. 1 '1 sing S' 0 0. 0
1.15267210D+15 3. 2 '2 trip S' 0 0. 0
9.60145430D+14 1. 2 '2 sing S' 0 0. 0
8.75933720D+14 9. 2 '2 trip P' 0 0. 0
8.14536220D+14 3. 2 '2 sing P' 0 0. 0
4.51727350D+14 3. 3 '3 trip S' 0 0. -103
4.02921120D+14 1. 3 '3 sing S' 0 0. -103
3.81935640D+14 9. 3 '3 trip P' 0 0. -103
3.65836790D+14 15. 3 '3 trip D' 0 0. -103
3.65746870D+14 5. 3 '3 sing D' 0 0. -103
3.62599020D+14 3. 3 '3 sing P' 0 0. -103
2.40043860D+14 3. 4 '4 trip S' 0 0. -104
2.20797190D+14 1. 4 '4 sing S' 0 0. -104
2.12492940D+14 9. 4 '4 trip P' 0 0. -104
2.05657660D+14 15. 4 '4 trip D' 0 0. -104
2.05597700D+14 5. 4 '4 sing D' 0 0. -104
2.05447800D+14 21. 4 '4 trip F' 0 0. -104
2.05447700D+14 7. 4 '4 sing F' 0 0. -104
2.04218650D+14 3. 4 '4 sing P' 0 0. -104
1.31522100D+14 75. 5 '<5 trip>' 0 0. -104
1.31521900D+14 25. 5 '<5 sing>' 0 0. -104
9.13347220D+13 144. 6 '<n=6> ' 0 0. -104
6.71030610D+13 196. 7 '<n=7> ' 0 0. -104
5.13757810D+13 256. 8 '<n=8> ' 0 0. -104
****** Continuum transitions
1 25 5 11 0 0 0 1.64 0.
5.89D15
2 25 1 13 0 0 0 16.8 0.
3 25 1 11 0 0 0 22.9 0.
4 25 1 13 0 0 0 17.5 0.
5 25 1 11 0 0 0 20.4 0.
6 25 1 13 0 0 0 85.0 0.
7 25 1 11 0 0 0 102. 0.
8 25 1 13 0 0 0 94.5 0.
9 25 1 13 0 0 0 52.5 0.
10 25 1 11 0 0 0 52.5 0.
11 25 1 11 0 0 0 105. 0.
12 25 1 13 0 0 0 249. 0.
13 25 1 11 0 0 0 288. 0.
14 25 1 13 0 0 0 288. 0.
15 25 1 13 0 0 0 219. 0.
16 25 1 11 0 0 0 219. 0.
17 25 1 13 0 0 0 88.5 0.
18 25 1 11 0 0 0 88.5 0.
19 25 1 11 0 0 0 304. 0.
20 25 1 0 0 0 0 365. 0.
21 25 1 0 0 0 0 365. 0.
22 25 1 0 0 0 0 626. 0.
23 25 1 0 0 0 0 995. 0.
24 25 1 0 0 0 0 1485. 0.
****** Line transitions
1 2 0 0 1 0 0 0. 0. ! He I lines
1 3 0 0 1 0 0 0. 0.
1 4 0 0 1 0 0 0. 0.
1 5 -1 1 1 0 0 0.2762 0.
T 3 29 400. 0.
0. 2.2E-6 0. 0. 0.
1 6 0 0 1 0 0 0. 0.
1 7 0 0 1 0 0 0. 0.
1 8 0 0 1 0 0 0. 0.
1 9 0 0 1 0 0 0. 0.
1 10 0 0 1 0 0 0. 0.
1 11 -1 1 1 0 0 0.0734 0.
T 3 23 200. 0.
0. 4.9E-5 0. 0. 0.
1 12 0 0 1 0 0 0. 0.
1 13 0 0 1 0 0 0. 0.
1 14 0 0 1 0 0 0. 0.
1 15 0 0 1 0 0 0. 0.
1 16 0 0 1 0 0 0. 0.
1 17 0 0 1 0 0 0. 0.
1 18 0 0 1 0 0 0. 0.
1 19 -1 1 1 0 0 0.0302 0.
T 3 23 200. 0.
0. 2.1E-4 0. 0. 0.
1 20 0 0 0 0 0 0. 0.
1 21 -1 0 0 0 0 0.0153 0.
F 1 7 0. 0.
1 22 -1 0 0 0 0 8.48d-3 0.
F 1 7 0. 0.
1 23 -1 0 0 0 0 5.93d-3 0.
F 1 7 0. 0.
1 24 -1 0 0 0 0 3.99d-3 0.
F 1 7 0. 0.
2 3 0 0 1 0 0 0. 0.
2 4 -1 1 1 0 0 0.5391 0.
T 3 11 40. 0.
0. 2.4E-6 0. 0. 0.
2 5 0 0 1 0 0 0. 0.
2 6 0 0 1 0 0 0. 0.
2 7 0 0 1 0 0 0. 0.
2 8 -1 1 1 0 0 0.06446 0.
T 3 11 40. 0.
0. 2.9E-5 0. 0. 0.
2 9 0 0 1 0 0 0. 0.
2 10 0 0 1 0 0 0. 0.
2 11 0 0 1 0 0 0. 0.
2 12 0 0 1 0 0 0. 0.
2 13 0 0 1 0 0 0. 0.
2 14 -1 1 1 0 0 0.0231 0.
T 3 11 40. 0.
0. 1.3E-4 0. 0. 0.
2 15 0 0 1 0 0 0. 0.
2 16 0 0 1 0 0 0. 0.
2 17 0 0 1 0 0 0. 0.
2 18 0 0 1 0 0 0. 0.
2 19 0 0 1 0 0 0. 0.
2 20 -1 0 0 0 0 0.0114 0.
F 1 7 0. 0.
2 21 0 0 0 0 0 0. 0.
2 22 -1 0 0 0 0 6.08d-3 0.
F 1 7 0. 0.
2 23 -1 0 0 0 0 3.81d-3 0.
F 1 7 0. 0.
2 24 -1 0 0 0 0 2.60d-3 0.
F 1 7 0. 0.
3 4 0 0 1 0 0 0. 0.
3 5 -1 1 1 0 0 0.3764 0.
T 3 11 40. 0.
0. 4.6E-6 0. 0. 0.
3 6 0 0 1 0 0 0. 0.
3 7 0 0 1 0 0 0. 0.
3 8 0 0 1 0 0 0. 0.
3 9 0 0 1 0 0 0. 0.
3 10 0 0 1 0 0 0. 0.
3 11 -1 1 1 0 0 0.1514 0.
T 3 11 40. 0.
0. 5.0E-5 0. 0. 0.
3 12 0 0 1 0 0 0. 0.
3 13 0 0 1 0 0 0. 0.
3 14 0 0 1 0 0 0. 0.
3 15 0 0 1 0 0 0. 0.
3 16 0 0 1 0 0 0. 0.
3 17 0 0 1 0 0 0. 0.
3 18 0 0 1 0 0 0. 0.
3 19 -1 1 1 0 0 0.0507 0.
T 3 11 40. 0.
0. 2.1E-4 0. 0. 0.
3 20 0 0 0 0 0 0. 0.
3 21 -1 0 0 0 0 0.0221 0.
F 1 7 0. 0.
3 22 -1 0 0 0 0 0.0128 0.
F 1 7 0. 0.
3 23 -1 0 0 0 0 0.0066 0.
F 1 7 0. 0.
3 24 -1 0 0 0 0 0.0044 0.
F 1 7 0. 0.
4 5 0 0 1 0 0 0. 0.
4 6 -1 1 1 0 0 0.0693 0.
T 3 11 40. 0.
0. 1.8E-5 0. 0. 0.
4 7 0 0 1 0 0 0. 0.
4 8 0 0 1 0 0 0. 0.
4 9 -1 1 1 0 0 0.6090 0.
T 3 11 40. 0.
0. 1.9E-5 0. 0. 0.
4 10 0 0 1 0 0 0. 0.
4 11 0 0 1 0 0 0. 0.
4 12 -1 1 1 0 0 0.0118 0.
T 3 11 40. 0.
0. 7.4E-5 0. 0. 0.
4 13 0 0 1 0 0 0. 0.
4 14 0 0 1 0 0 0. 0.
4 15 -1 1 1 0 0 0.125 0.
T 3 15 80. 0.
0. 2.0E-4 0. 0. 0.
4 16 0 0 1 0 0 0. 0.
4 17 0 0 1 0 0 0. 0.
4 18 0 0 1 0 0 0. 0.
4 19 0 0 1 0 0 0. 0.
4 20 -1 0 0 0 0 5.105d-2 0.
F 1 7 0. 0.
4 21 0 0 0 0 0 0. 0.
4 22 -1 0 0 0 0 2.326d-2 0.
F 1 7 0. 0.
4 23 -1 0 0 0 0 1.520d-2 0.
F 1 7 0. 0.
4 24 -1 0 0 0 0 9.341d-3 0.
F 1 7 0. 0.
5 6 0 0 1 0 0 0. 0.
5 7 -1 1 1 0 0 0.0480 0.
T 3 11 40. 0.
0. 2.9E-5 0. 0. 0.
5 8 0 0 1 0 0 0. 0.
5 9 0 0 1 0 0 0. 0.
5 10 -1 1 1 0 0 0.7110 0.
T 3 11 40. 0.
0. 3.0E-5 0. 0. 0.
5 11 0 0 1 0 0 0. 0.
5 12 0 0 1 0 0 0. 0.
5 13 -1 1 1 0 0 0.00834 0.
T 3 11 40. 0.
0. 1.1E-4 0. 0. 0.
5 14 0 0 1 0 0 0. 0.
5 15 0 0 1 0 0 0. 0.
5 16 -1 1 1 0 0 0.122 0.
T 3 11 40. 0.
0. 2.5E-4 0. 0. 0.
5 17 0 0 1 0 0 0. 0.
5 18 0 0 1 0 0 0. 0.
5 19 0 0 1 0 0 0. 0.
5 20 0 0 0 0 0 0. 0.
5 21 -1 0 0 0 0 4.688d-2 0.
F 1 7 0. 0.
5 22 -1 0 0 0 0 2.283d-2 0.
F 1 7 0. 0.
5 23 -1 0 0 0 0 1.208d-2 0.
F 1 7 0. 0.
5 24 -1 0 0 0 0 8.056d-3 0.
F 1 7 0. 0.
6 7 0 0 1 0 0 0. 0.
6 8 -1 0 1 0 0 0.896 0.
F 1 7 0. 0.
6 9 0 0 1 0 0 0. 0.
6 10 0 0 1 0 0 0. 0.
6 11 0 0 1 0 0 0. 0.
6 12 0 0 1 0 0 0. 0.
6 13 0 0 1 0 0 0. 0.
6 14 -1 0 1 0 0 0.0429 0.
F 1 7 0. 0.
6 15 0 0 1 0 0 0. 0.
6 16 0 0 1 0 0 0. 0.
6 17 0 0 1 0 0 0. 0.
6 18 0 0 1 0 0 0. 0.
6 19 0 0 1 0 0 0. 0.
6 20 -1 0 0 0 0 0.0245 0.
F 1 7 0. 0.
6 21 0 0 0 0 0 0. 0.
6 22 -1 0 0 0 0 2.25e-3 0.
F 1 7 0. 0.
6 23 -1 0 0 0 0 1.5e-3 0.
F 1 7 0. 0.
6 24 -1 0 0 0 0 1.0e-3 0.
F 1 7 0. 0.
7 8 0 0 1 0 0 0. 0.
7 9 0 0 1 0 0 0. 0.
7 10 0 0 1 0 0 0. 0.
7 11 -1 0 1 0 0 0.629 0.
F 1 7 0. 0.
7 12 0 0 1 0 0 0. 0.
7 13 0 0 1 0 0 0. 0.
7 14 0 0 1 0 0 0. 0.
7 15 0 0 1 0 0 0. 0.
7 16 0 0 1 0 0 0. 0.
7 17 0 0 1 0 0 0. 0.
7 18 0 0 1 0 0 0. 0.
7 19 -1 0 1 0 0 0.140 0.
F 1 7 0. 0.
7 20 0 0 0 0 0 0. 0.
7 21 -1 0 0 0 0 0.0521 0.
F 1 7 0. 0.
7 22 -1 0 0 0 0 0.0234 0.
F 1 7 0. 0.
7 23 -1 0 0 0 0 0.0156 0.
F 1 7 0. 0.
7 24 -1 0 0 0 0 0.0104 0.
F 1 7 0. 0.
8 9 -1 0 1 0 0 0.111 0.
F 1 7 0. 0.
8 10 0 0 1 0 0 0. 0.
8 11 0 0 1 0 0 0. 0.
8 12 -1 0 1 0 0 0.145 0.
F 1 7 0. 0.
8 13 0 0 1 0 0 0. 0.
8 14 0 0 1 0 0 0. 0.
8 15 -1 0 1 0 0 0.482 0.
F 1 7 0. 0.
8 16 0 0 1 0 0 0. 0.
8 17 0 0 1 0 0 0. 0.
8 18 0 0 1 0 0 0. 0.
8 19 0 0 1 0 0 0. 0.
8 20 -1 0 0 0 0 0.1452 0.
F 1 7 0. 0.
8 21 0 0 0 0 0 0. 0.
8 22 -1 0 0 0 0 0.0028 0.
F 1 7 0. 0.
8 23 -1 0 0 0 0 0.00187 0.
F 1 7 0. 0.
8 24 -1 0 0 0 0 0.00124 0.
F 1 7 0. 0.
9 10 0 0 1 0 0 0. 0.
9 11 0 0 1 0 0 0. 0.
9 12 0 0 1 0 0 0. 0.
9 13 0 0 1 0 0 0. 0.
9 14 -1 0 1 0 0 0.0205 0.
F 1 7 0. 0.
9 15 0 0 1 0 0 0. 0.
9 16 0 0 1 0 0 0. 0.
9 17 -1 0 1 0 0 1.02 0.
F 1 7 0. 0.
9 18 0 0 1 0 0 0. 0.
9 19 0 0 1 0 0 0. 0.
9 20 -1 0 0 0 0 0.1622 0.
F 1 7 0. 0.
9 21 0 0 0 0 0 0. 0.
9 22 -1 0 0 0 0 0.0537 0.
F 1 7 0. 0.
9 23 -1 0 0 0 0 0.0358 0.
F 1 7 0. 0.
9 24 -1 0 0 0 0 0.0239 0.
F 1 7 0. 0.
10 11 -1 0 1 0 0 0.0139 0.
F 1 7 0. 0.
10 12 0 0 1 0 0 0. 0.
10 13 0 0 1 0 0 0. 0.
10 14 0 0 1 0 0 0. 0.
10 15 0 0 1 0 0 0. 0.
10 16 0 0 1 0 0 0. 0.
10 17 0 0 1 0 0 0. 0.
10 18 -1 0 1 0 0 1.01 0.
F 1 7 0. 0.
10 19 -1 0 1 0 0 8.58e-3 0.
F 1 7 0. 0.
10 20 0 0 0 0 0 0. 0.
10 21 -1 0 0 0 0 0.1599 0.
F 1 7 0. 0.
10 22 -1 0 0 0 0 0.0539 0.
F 1 7 0. 0.
10 23 -1 0 0 0 0 0.0359 0.
F 1 7 0. 0.
10 24 -1 0 0 0 0 0.0240 0.
F 1 7 0. 0.
11 12 0 0 1 0 0 0. 0.
11 13 -1 0 1 0 0 0.103 0.
F 1 7 0. 0.
11 14 0 0 1 0 0 0. 0.
11 15 0 0 1 0 0 0. 0.
11 16 -1 0 1 0 0 0.647 0.
F 1 7 0. 0.
11 17 0 0 1 0 0 0. 0.
11 18 0 0 1 0 0 0. 0.
11 19 0 0 1 0 0 0. 0.
11 20 0 0 0 0 0 0. 0.
11 21 -1 0 0 0 0 0.1572 0.
F 1 7 0. 0.
11 22 -1 0 0 0 0 0.0622 0.
F 1 7 0. 0.
11 23 -1 0 0 0 0 0.0415 0.
F 1 7 0. 0.
11 24 -1 0 0 0 0 0.0276 0.
F 1 7 0. 0.
12 13 0 0 1 0 0 0. 0.
12 14 -1 0 1 0 0 1.21 0.
F 1 7 0. 0.
12 15 0 0 1 0 0 0. 0.
12 16 0 0 1 0 0 0. 0.
12 17 0 0 1 0 0 0. 0.
12 18 0 0 1 0 0 0. 0.
12 19 0 0 1 0 0 0. 0.
12 20 -1 0 0 0 0 0.0468 0.
F 1 7 0. 0.
12 21 0 0 0 0 0 0. 0.
12 22 -1 0 0 0 0 0.0276 0.
F 1 7 0. 0.
12 23 -1 0 0 0 0 0.0184 0.
F 1 7 0. 0.
12 24 -1 0 0 0 0 0.0123 0.
F 1 7 0. 0.
13 14 0 0 1 0 0 0. 0.
13 15 0 0 1 0 0 0. 0.
13 16 0 0 1 0 0 0. 0.
13 17 0 0 1 0 0 0. 0.
13 18 0 0 1 0 0 0. 0.
13 19 -1 0 1 0 0 0.853 0.
F 1 7 0. 0.
13 20 0 0 0 0 0 0. 0.
13 21 -1 0 0 0 0 0.151 0.
F 1 7 0. 0.
13 22 -1 0 0 0 0 0.0599 0.
F 1 7 0. 0.
13 23 -1 0 0 0 0 0.0399 0.
F 1 7 0. 0.
13 24 -1 0 0 0 0 0.0266 0.
F 1 7 0. 0.
14 15 -1 0 1 0 0 0.200 0.
F 1 7 0. 0.
14 16 0 0 1 0 0 0. 0.
14 17 0 0 1 0 0 0. 0.
14 18 0 0 1 0 0 0. 0.
14 19 0 0 1 0 0 0. 0.
14 20 -1 0 0 0 0 0.665 0.
F 1 7 0. 0.
14 21 0 0 0 0 0 0. 0.
14 22 -1 0 0 0 0 0.1544 0.
F 1 7 0. 0.
14 23 -1 0 0 0 0 0.1029 0.
F 1 7 0. 0.
14 24 -1 0 0 0 0 0.0686 0.
F 1 7 0. 0.
15 16 0 0 1 0 0 0. 0.
15 17 -1 0 1 0 0 3.31e-3 0.
F 1 7 0. 0.
15 18 0 0 1 0 0 0. 0.
15 19 0 0 1 0 0 0. 0.
15 20 -1 0 0 0 0 0.942 0.
F 1 7 0. 0.
15 21 0 0 0 0 0 0. 0.
15 22 -1 0 0 0 0 0.197 0.
F 1 7 0. 0.
15 23 -1 0 0 0 0 0.131 0.
F 1 7 0. 0.
15 24 -1 0 0 0 0 0.088 0.
F 1 7 0. 0.
16 17 0 0 1 0 0 0. 0.
16 18 -1 0 1 0 0 2.53e-3 0.
F 1 7 0. 0.
16 19 0 0 1 0 0 0. 0.
16 20 0 0 0 0 0 0. 0.
16 21 -1 0 0 0 0 0.911 0.
F 1 7 0. 0.
16 22 -1 0 0 0 0 0.192 0.
F 1 7 0. 0.
16 23 -1 0 0 0 0 0.128 0.
F 1 7 0. 0.
16 24 -1 0 0 0 0 0.085 0.
F 1 7 0. 0.
17 18 0 0 1 0 0 0. 0.
17 19 0 0 1 0 0 0. 0.
17 20 0 0 0 0 0 0. 0.
17 21 0 0 0 0 0 0. 0.
17 22 0 0 0 0 0 0. 0.
17 23 0 0 0 0 0 0. 0.
17 24 0 0 0 0 0 0. 0.
18 19 0 0 1 0 0 0. 0.
18 20 0 0 0 0 0 0. 0.
18 21 0 0 0 0 0 0. 0.
18 22 0 0 0 0 0 0. 0.
18 23 0 0 0 0 0 0. 0.
18 24 0 0 0 0 0 0. 0.
19 20 0 0 0 0 0 0. 0.
19 21 -1 0 0 0 0 0.808 0.
F 1 7 0. 0.
19 22 -1 0 0 0 0 0.1794 0.
F 1 7 0. 0.
19 23 -1 0 0 0 0 0.1196 0.
F 1 7 0. 0.
19 24 -1 0 0 0 0 0.0797 0.
F 1 7 0. 0.
20 22 0 0 0 0 0 0. 0.
20 23 0 0 0 0 0 0. 0.
20 24 0 0 0 0 0 0. 0.
21 22 0 0 0 0 0 0. 0.
21 23 0 0 0 0 0 0. 0.
21 24 0 0 0 0 0 0. 0.
22 23 0 0 0 0 0 0. 0.
22 24 0 0 0 0 0 0. 0.
23 24 0 0 0 0 0 0. 0.
+356
View File
@@ -0,0 +1,356 @@
****** Levels
1.31575977D+16 0. 1 ' (N=1) ' 1 0. 0
3.28939942D+15 0. 2 ' (N=2) ' 1 0. 0
1.46195530D+15 0. 3 ' (N=3) ' 1 0. 0
8.22349855D+14 0. 4 ' (N=4) ' 1 0. 0
5.26303907D+14 0. 5 ' (N=5) ' 1 0. -111
3.65488824D+14 0. 6 ' (N=6) ' 1 0. -111
2.68522402D+14 0. 7 ' (N=7) ' 1 0. -111
2.05587464D+14 0. 8 ' (N=8) ' 1 0. -111
1.62439477D+14 0. 9 ' (N=9) ' 1 0. -111
1.31575977D+14 0. 10 ' (N=10) ' 1 0. -111
1.08740477D+14 0. 11 ' (N=11) ' 1 0. -111
9.13722061D+13 0. 12 ' (N=12) ' 1 0. -111
7.78556075D+13 0. 13 ' (N=13) ' 1 0. -111
6.71306004D+13 0. 14 ' (N=14) ' 1 0. -111
5.84782120D+13 0. 15 ' (N=15) ' 1 0. -111
5.13968660D+13 0. 16 ' (N=16) ' 1 0. -111
4.55280197D+13 0. 17 ' (N=17) ' 1 0. -111
4.06098694D+13 0. 18 ' (N=18) ' 1 0. -111
3.64476391D+13 0. 19 ' (N=19) ' 1 0. -111
3.28939942D+13 0. 20 ' (N=20) ' 1 0. -111
****** Continuum transitions
1 21 5 1 0 1 3 0. 0.
1.D+16
2 21 5 1 0 0 0 0. 0.
2.6D+15
3 21 1 1 0 0 0 0. 0.
4 21 1 1 0 0 0 0. 0.
5 21 1 1 0 0 0 0. 0.
6 21 1 1 0 0 0 0. 0.
7 21 1 1 0 0 0 0. 0.
8 21 1 1 0 0 0 0. 0.
9 21 1 1 0 0 0 0. 0.
10 21 1 1 0 0 0 0. 0.
11 21 1 1 0 0 0 0. 0.
12 21 1 1 0 0 0 0. 0.
13 21 1 1 0 0 0 0. 0.
14 21 1 1 0 0 0 0. 0.
15 21 1 1 0 0 0 0. 0.
16 21 1 1 0 0 0 0. 0.
17 21 1 1 0 0 0 0. 0.
18 21 1 1 0 0 0 0. 0.
19 21 1 1 0 0 0 0. 0.
20 21 1 1 0 0 0 0. 0.
****** Line transitions
1 2 -1 2 0 0 0 0. 0.
T 3 17 510. 0.
1 3 -1 2 0 0 0 0. 0.
T 3 17 510. 0.
1 4 -1 2 0 0 0 0. 0.
T 3 17 510. 0.
1 5 -1 2 0 0 0 0. 0.
T 3 17 510. 0.
1 6 -1 2 0 0 0 0. 0.
T 3 15 254. 0.
1 7 -1 2 0 0 0 0. 0.
T 3 15 254. 0.
1 8 -1 2 0 0 0 0. 0.
T 3 15 254. 0.
1 9 -1 2 0 0 0 0. 0.
T 3 15 254. 0.
1 10 -1 2 0 0 0 0. 0.
T 3 15 254. 0.
1 11 -1 2 0 0 0 0. 0.
T 3 15 254. 0.
1 12 -1 2 0 0 0 0. 0.
T 3 15 254. 0.
1 13 -1 2 0 0 0 0. 0.
T 3 15 254. 0.
1 14 -1 2 0 0 0 0. 0.
T 3 15 254. 0.
1 15 -1 2 0 0 0 0. 0.
T 3 15 254. 0.
1 16 -1 2 0 0 0 0. 0.
T 3 15 254. 0.
1 17 -1 2 0 0 0 0. 0.
T 3 15 254. 0.
1 18 -1 2 0 0 0 0. 0.
T 3 15 254. 0.
1 19 -1 2 0 0 0 0. 0.
T 3 15 254. 0.
1 20 -1 2 0 0 0 0. 0.
T 3 15 254. 0.
2 3 -1 2 0 0 0 0. 0. ! He II Balmer-alpha
T 3 17 510. 0.
2 4 -1 2 0 0 0 0. 0.
T 3 17 510. 0.
2 5 -1 2 0 0 0 0. 0.
T 3 15 254. 0.
2 6 -1 2 0 0 0 0. 0.
T 3 15 254. 0.
2 7 -1 2 0 0 0 0. 0.
T 3 15 254. 0.
2 8 -1 2 0 0 0 0. 0.
T 3 15 254. 0.
2 9 -1 2 0 0 0 0. 0.
T 3 13 126. 0.
2 10 -1 2 0 0 0 0. 0.
T 3 13 126. 0.
2 11 -1 2 0 0 0 0. 0.
T 3 13 126. 0.
2 12 -1 2 0 0 0 0. 0.
T 3 13 126. 0.
2 13 -1 2 0 0 0 0. 0.
T 3 13 126. 0.
2 14 -1 2 0 0 0 0. 0.
T 3 13 126. 0.
2 15 -1 2 0 0 0 0. 0.
T 3 13 126. 0.
2 16 -1 2 0 0 0 0. 0.
T 3 13 126. 0.
2 17 -1 2 0 0 0 0. 0.
T 3 13 126. 0.
2 18 -1 2 0 0 0 0. 0.
T 3 13 126. 0.
2 19 -1 2 0 0 0 0. 0.
T 3 13 126. 0.
2 20 -1 2 0 0 0 0. 0.
T 3 13 126. 0.
3 4 -1 2 0 0 0 0. 0.
T 3 17 510. 0.
3 5 -1 2 0 0 0 0. 0.
T 3 15 254. 0.
3 6 -1 2 0 0 0 0. 0.
T 3 15 254. 0.
3 7 -1 2 0 0 0 0. 0.
T 3 15 254. 0.
3 8 -1 2 0 0 0 0. 0.
T 3 15 254. 0.
3 9 -1 2 0 0 0 0. 0.
T 3 13 126. 0.
3 10 -1 2 0 0 0 0. 0.
T 3 13 126. 0.
3 11 -1 2 0 0 0 0. 0.
T 3 13 126. 0.
3 12 -1 2 0 0 0 0. 0.
T 3 13 126. 0.
3 13 -1 2 0 0 0 0. 0.
T 3 13 126. 0.
3 14 -1 2 0 0 0 0. 0.
T 3 13 126. 0.
3 15 -1 2 0 0 0 0. 0.
T 3 13 126. 0.
3 16 -1 2 0 0 0 0. 0.
T 3 13 126. 0.
3 17 -1 2 0 0 0 0. 0.
T 3 13 126. 0.
3 18 -1 2 0 0 0 0. 0.
T 3 13 126. 0.
3 19 -1 2 0 0 0 0. 0.
T 3 13 126. 0.
3 20 -1 2 0 0 0 0. 0.
T 3 13 126. 0.
4 5 -1 2 0 0 0 0. 0.
T 3 15 254. 0.
4 6 -1 2 0 0 0 0. 0.
T 3 15 254. 0.
4 7 -1 2 0 0 0 0. 0.
T 3 13 126. 0.
4 8 -1 2 0 0 0 0. 0.
T 3 13 126. 0.
4 9 -1 2 0 0 0 0. 0.
T 3 13 126. 0.
4 10 -1 2 0 0 0 0. 0.
T 3 13 126. 0.
4 11 -1 2 0 0 0 0. 0.
T 3 13 126. 0.
4 12 -1 2 0 0 0 0. 0.
T 3 13 126. 0.
4 13 -1 2 0 0 0 0. 0.
T 3 13 126. 0.
4 14 -1 2 0 0 0 0. 0.
T 3 13 126. 0.
4 15 -1 2 0 0 0 0. 0.
T 3 13 126. 0.
4 16 -1 2 0 0 0 0. 0.
T 3 13 126. 0.
4 17 -1 2 0 0 0 0. 0.
T 3 13 126. 0.
4 18 -1 2 0 0 0 0. 0.
T 3 13 126. 0.
4 19 -1 2 0 0 0 0. 0.
T 3 13 126. 0.
4 20 -1 2 0 0 0 0. 0.
T 3 13 126. 0.
5 6 -1 0 0 0 0 0. 0.
F 1 7 0. 0.
5 7 -1 0 0 0 0 0. 0.
F 1 7 0. 0.
5 8 -1 0 0 0 0 0. 0.
F 1 7 0. 0.
5 9 -1 0 0 0 0 0. 0.
F 1 7 0. 0.
5 10 -1 0 0 0 0 0. 0.
F 1 7 0. 0.
5 11 -1 0 0 0 0 0. 0.
F 1 7 0. 0.
5 12 -1 0 0 0 0 0. 0.
F 1 7 0. 0.
5 13 -1 0 0 0 0 0. 0.
F 1 7 0. 0.
5 14 -1 0 0 0 0 0. 0.
F 1 7 0. 0.
5 15 -1 0 0 0 0 0. 0.
F 1 7 0. 0.
5 16 -1 0 0 0 0 0. 0.
F 1 7 0. 0.
5 17 -1 0 0 0 0 0. 0.
F 1 7 0. 0.
5 18 -1 0 0 0 0 0. 0.
F 1 7 0. 0.
5 19 -1 0 0 0 0 0. 0.
F 1 7 0. 0.
5 20 -1 0 0 0 0 0. 0.
F 1 7 0. 0.
6 7 -1 0 0 0 0 0. 0.
F 1 7 0. 0.
6 8 -1 0 0 0 0 0. 0.
F 1 7 0. 0.
6 9 -1 0 0 0 0 0. 0.
F 1 7 0. 0.
6 10 -1 0 0 0 0 0. 0.
F 1 7 0. 0.
6 11 -1 0 0 0 0 0. 0.
F 1 7 0. 0.
6 12 -1 0 0 0 0 0. 0.
F 1 7 0. 0.
6 13 -1 0 0 0 0 0. 0.
F 1 7 0. 0.
6 14 -1 0 0 0 0 0. 0.
F 1 7 0. 0.
6 15 -1 0 0 0 0 0. 0.
F 1 7 0. 0.
6 16 -1 0 0 0 0 0. 0.
F 1 7 0. 0.
6 17 -1 0 0 0 0 0. 0.
F 1 7 0. 0.
6 18 -1 0 0 0 0 0. 0.
F 1 7 0. 0.
6 19 -1 0 0 0 0 0. 0.
F 1 7 0. 0.
6 20 -1 0 0 0 0 0. 0.
F 1 7 0. 0.
7 8 -1 0 0 0 0 0. 0.
F 1 7 0. 0.
7 9 -1 0 0 0 0 0. 0.
F 1 7 0. 0.
7 10 -1 0 0 0 0 0. 0.
F 1 7 0. 0.
7 11 -1 0 0 0 0 0. 0.
F 1 7 0. 0.
7 12 -1 0 0 0 0 0. 0.
F 1 7 0. 0.
7 13 -1 0 0 0 0 0. 0.
F 1 7 0. 0.
7 14 -1 0 0 0 0 0. 0.
F 1 7 0. 0.
7 15 0 0 0 0 0 0. 0.
7 16 0 0 0 0 0 0. 0.
7 17 0 0 0 0 0 0. 0.
7 18 0 0 0 0 0 0. 0.
7 19 0 0 0 0 0 0. 0.
7 20 0 0 0 0 0 0. 0.
8 9 -1 0 0 0 0 0. 0.
F 1 7 0. 0.
8 10 -1 0 0 0 0 0. 0.
F 1 7 0. 0.
8 11 -1 0 0 0 0 0. 0.
F 1 7 0. 0.
8 12 -1 0 0 0 0 0. 0.
F 1 7 0. 0.
8 13 -1 0 0 0 0 0. 0.
F 1 7 0. 0.
8 14 -1 0 0 0 0 0. 0.
F 1 7 0. 0.
8 15 0 0 0 0 0 0. 0.
8 16 0 0 0 0 0 0. 0.
8 17 0 0 0 0 0 0. 0.
8 18 0 0 0 0 0 0. 0.
8 19 0 0 0 0 0 0. 0.
8 20 0 0 0 0 0 0. 0.
9 10 -1 0 0 0 0 0. 0.
F 1 7 0. 0.
9 11 -1 0 0 0 0 0. 0.
F 1 7 0. 0.
9 12 -1 0 0 0 0 0. 0.
F 1 7 0. 0.
9 13 -1 0 0 0 0 0. 0.
F 1 7 0. 0.
9 14 -1 0 0 0 0 0. 0.
F 1 7 0. 0.
9 15 0 0 0 0 0 0. 0.
9 16 0 0 0 0 0 0. 0.
9 17 0 0 0 0 0 0. 0.
9 18 0 0 0 0 0 0. 0.
9 19 0 0 0 0 0 0. 0.
9 20 0 0 0 0 0 0. 0.
10 11 -1 0 0 0 0 0. 0.
F 1 7 0. 0.
10 12 -1 0 0 0 0 0. 0.
F 1 7 0. 0.
10 13 -1 0 0 0 0 0. 0.
F 1 7 0. 0.
10 14 -1 0 0 0 0 0. 0.
F 1 7 0. 0.
10 15 0 0 0 0 0 0. 0.
10 16 0 0 0 0 0 0. 0.
10 17 0 0 0 0 0 0. 0.
10 18 0 0 0 0 0 0. 0.
10 19 0 0 0 0 0 0. 0.
10 20 0 0 0 0 0 0. 0.
11 12 0 0 0 0 0 0. 0.
11 13 0 0 0 0 0 0. 0.
11 14 0 0 0 0 0 0. 0.
11 15 0 0 0 0 0 0. 0.
11 16 0 0 0 0 0 0. 0.
11 17 0 0 0 0 0 0. 0.
11 18 0 0 0 0 0 0. 0.
11 19 0 0 0 0 0 0. 0.
11 20 0 0 0 0 0 0. 0.
12 13 0 0 0 0 0 0. 0.
12 14 0 0 0 0 0 0. 0.
12 15 0 0 0 0 0 0. 0.
12 16 0 0 0 0 0 0. 0.
12 17 0 0 0 0 0 0. 0.
12 18 0 0 0 0 0 0. 0.
12 19 0 0 0 0 0 0. 0.
12 20 0 0 0 0 0 0. 0.
13 14 0 0 0 0 0 0. 0.
13 15 0 0 0 0 0 0. 0.
13 16 0 0 0 0 0 0. 0.
13 17 0 0 0 0 0 0. 0.
13 18 0 0 0 0 0 0. 0.
13 19 0 0 0 0 0 0. 0.
13 20 0 0 0 0 0 0. 0.
14 15 0 0 0 0 0 0. 0.
14 16 0 0 0 0 0 0. 0.
14 17 0 0 0 0 0 0. 0.
14 18 0 0 0 0 0 0. 0.
14 19 0 0 0 0 0 0. 0.
14 20 0 0 0 0 0 0. 0.
15 16 0 0 0 0 0 0. 0.
15 17 0 0 0 0 0 0. 0.
15 18 0 0 0 0 0 0. 0.
15 19 0 0 0 0 0 0. 0.
15 20 0 0 0 0 0 0. 0.
16 17 0 0 0 0 0 0. 0.
16 18 0 0 0 0 0 0. 0.
16 19 0 0 0 0 0 0. 0.
16 20 0 0 0 0 0 0. 0.
17 18 0 0 0 0 0 0. 0.
17 19 0 0 0 0 0 0. 0.
17 20 0 0 0 0 0 0. 0.
18 19 0 0 0 0 0 0. 0.
18 20 0 0 0 0 0 0. 0.
19 20 0 0 0 0 0 0. 0.
+578
View File
@@ -0,0 +1,578 @@
****** Levels
3.63542326E+15 2. 3 'MgII 2Se 1' 0 0. 0
2.56617284E+15 2. 3 'MgII 2Po 1' 0 0. 0
2.56342764E+15 4. 3 'MgII 2Po 1' 0 0. 0
1.54277601E+15 2. 3 'MgII 2Se 2' 0 0. 0
1.49224505E+15 10. 3 'MgII 2De 1' 0 0. 0
1.21796065E+15 6. 3 'MgII 2Po 2' 0 0. 0
8.53701120E+14 2. 4 'MgII 2Se 3' 0 0. -107
8.38104349E+14 10. 4 'MgII 2De 2' 0 0. -107
8.23448511E+14 14. 4 'MgII 2Fo 1' 0 0. -107
7.13590026E+14 6. 4 'MgII 2Po 3' 0 0. -107
5.41739123E+14 2. 5 'MgII 2Se 4' 0 0. -107
5.35051154E+14 10. 5 'MgII 2De 3' 0 0. -107
5.26954906E+14 14. 5 'MgII 2Fo 2' 0 0. -107
5.26481319E+14 18. 5 'MgII 2Ge 1' 0 0. -107
4.68874064E+14 6. 5 'MgII 2Po 4' 0 0. -107
3.74230768E+14 2. 6 'MgII 2Se 5' 0 0. -107
3.70760200E+14 10. 6 'MgII 2De 4' 0 0. -107
3.65897928E+14 14. 6 'MgII 2Fo 3' 0 0. -107
3.65604930E+14 18. 6 'MgII 2Ge 2' 0 0. -107
3.65549196E+14 22. 6 'MgII 2Ho 1' 0 0. -107
3.31595332E+14 6. 6 'MgII 2Po 5' 0 0. -107
2.67863202E+14 98. 7 'MgII+2__ 1' 0 0. -107
2.05231388E+14 128. 8 'MgII+2__ 2' 0 0. -107
1.62236702E+14 162. 9 'MgII+2__ 3' 0 0. -107
1.31676131E+14 194. 10 'MgII+2__ 4' 0 0. -107
****** Continuum transitions
1 26 1 107 0 0 0 4.012E-20 0.000E+00
-0.0162 0.0614 0.1261 0.2101 0.3136 0.4041 0.4229
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1.1273
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3.000 11.858 1.000 0.000
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0.9096 1.1618 1.2770
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0.003 1.066 1.520
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*** Line transitions
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T 3 25 1000. 0.
2.7E+8 2.1E-6 0. 0. 0.
1 3 -1 1 1 25 25 6.200E-01 7.000E-01
T 3 25 1000. 0.
2.7E+8 2.1E-6 0. 0. 0.
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12 18 -1 0 1 0 0 7.070E-01 2.000E-01
F 1 7 0. 0.
12 19 0 0 4 0 0 0.000E+00 5.000E-02
12 20 0 0 4 0 0 0.000E+00 5.000E-02
12 21 -1 0 1 0 0 1.460E-02 2.000E-01
F 1 7 0. 0.
12 22 -1 0 1 0 0 1.881E-01 2.000E-01
F 1 7 0. 0.
12 23 -1 0 1 0 0 8.085E-02 2.000E-01
F 1 7 0. 0.
12 24 -1 0 1 0 0 4.354E-02 2.000E-01
F 1 7 0. 0.
12 25 -1 0 1 0 0 2.600E-02 2.000E-01
F 1 7 0. 0.
13 14 0 0 4 0 0 0.000E+00 5.000E-02
13 15 0 0 4 0 0 0.000E+00 5.000E-02
13 16 0 0 4 0 0 0.000E+00 5.000E-02
13 17 -1 0 1 0 0 3.814E-02 2.000E-01
F 1 7 0. 0.
13 18 0 0 4 0 0 0.000E+00 5.000E-02
13 19 -1 0 1 0 0 1.591E+00 2.000E-01
F 1 7 0. 0.
13 20 0 0 4 0 0 0.000E+00 5.000E-02
13 21 0 0 4 0 0 0.000E+00 5.000E-02
13 22 -1 0 1 0 0 2.502E-01 2.000E-01
F 1 7 0. 0.
13 23 -1 0 1 0 0 8.714E-02 2.000E-01
F 1 7 0. 0.
13 24 -1 0 1 0 0 4.194E-02 2.000E-01
F 1 7 0. 0.
13 25 -1 0 1 0 0 2.395E-02 2.000E-01
F 1 7 0. 0.
14 15 0 0 4 0 0 0.000E+00 5.000E-02
14 16 0 0 4 0 0 0.000E+00 5.000E-02
14 17 0 0 4 0 0 0.000E+00 5.000E-02
14 18 -1 0 1 0 0 1.591E+00 2.000E-01
F 1 7 0. 0.
14 19 0 0 4 0 0 0.000E+00 5.000E-02
14 20 -1 0 1 0 0 1.591E+00 2.000E-01
F 1 7 0. 0.
14 21 0 0 4 0 0 0.000E+00 5.000E-02
14 22 -1 0 1 0 0 4.864E-01 2.000E-01
F 1 7 0. 0.
14 23 -1 0 1 0 0 1.692E-01 2.000E-01
F 1 7 0. 0.
14 24 -1 0 1 0 0 8.137E-02 2.000E-01
F 1 7 0. 0.
14 25 -1 0 1 0 0 4.647E-02 2.000E-01
F 1 7 0. 0.
15 16 -1 0 1 0 0 5.083E-01 2.000E-01
F 1 7 0. 0.
15 17 -1 0 1 0 0 1.767E+00 2.000E-01
F 1 7 0. 0.
15 18 0 0 4 0 0 0.000E+00 5.000E-02
15 19 0 0 4 0 0 0.000E+00 5.000E-02
15 20 0 0 4 0 0 0.000E+00 5.000E-02
15 21 0 0 4 0 0 0.000E+00 5.000E-02
15 22 -1 0 1 0 0 1.932E-01 2.000E-01
F 1 7 0. 0.
15 23 -1 0 1 0 0 5.733E-02 2.000E-01
F 1 7 0. 0.
15 24 -1 0 1 0 0 2.552E-02 2.000E-01
F 1 7 0. 0.
15 25 -1 0 1 0 0 1.393E-02 2.000E-01
F 1 7 0. 0.
16 17 0 0 4 0 0 0.000E+00 5.000E-02
16 18 0 0 4 0 0 0.000E+00 5.000E-02
16 19 0 0 4 0 0 0.000E+00 5.000E-02
16 20 0 0 4 0 0 0.000E+00 5.000E-02
16 21 -1 0 1 0 0 2.665E+00 7.000E-01
F 1 7 0. 0.
16 22 -1 0 1 0 0 1.615E-02 2.000E-01
F 1 7 0. 0.
16 23 -1 0 1 0 0 1.275E-03 2.000E-01
F 1 7 0. 0.
16 24 -1 0 1 0 0 1.735E-04 2.000E-01
F 1 7 0. 0.
16 25 0 0 4 0 0 0.000E+00 5.000E-02
17 18 -1 0 1 0 0 1.840E-01 7.000E-01
F 1 7 0. 0.
17 19 0 0 4 0 0 0.000E+00 5.000E-02
17 20 0 0 4 0 0 0.000E+00 5.000E-02
17 21 -1 0 1 0 0 7.040E-01 7.000E-01
F 1 7 0. 0.
17 22 -1 0 1 0 0 6.931E-01 2.000E-01
F 1 7 0. 0.
17 23 -1 0 1 0 0 1.890E-01 2.000E-01
F 1 7 0. 0.
17 24 -1 0 1 0 0 8.365E-02 2.000E-01
F 1 7 0. 0.
17 25 -1 0 1 0 0 4.470E-02 2.000E-01
F 1 7 0. 0.
18 19 0 0 4 0 0 0.000E+00 5.000E-02
18 20 0 0 4 0 0 0.000E+00 5.000E-02
18 21 0 0 4 0 0 0.000E+00 5.000E-02
18 22 -1 0 1 0 0 1.902E+00 2.000E-01
F 1 7 0. 0.
18 23 -1 0 1 0 0 2.868E-01 2.000E-01
F 1 7 0. 0.
18 24 -1 0 1 0 0 9.873E-02 2.000E-01
F 1 7 0. 0.
18 25 -1 0 1 0 0 4.717E-02 2.000E-01
F 1 7 0. 0.
19 20 0 0 4 0 0 0.000E+00 5.000E-02
19 21 0 0 4 0 0 0.000E+00 5.000E-02
19 22 -1 0 1 0 0 3.673E+00 2.000E-01
F 1 7 0. 0.
19 23 -1 0 1 0 0 5.486E-01 2.000E-01
F 1 7 0. 0.
19 24 -1 0 1 0 0 1.882E-01 2.000E-01
F 1 7 0. 0.
19 25 -1 0 1 0 0 8.973E-02 2.000E-01
F 1 7 0. 0.
20 21 0 0 4 0 0 0.000E+00 5.000E-02
20 22 -1 0 1 0 0 3.673E+00 2.000E-01
F 1 7 0. 0.
20 23 -1 0 1 0 0 5.486E-01 2.000E-01
F 1 7 0. 0.
20 24 -1 0 1 0 0 1.882E-01 2.000E-01
F 1 7 0. 0.
20 25 -1 0 1 0 0 8.973E-02 2.000E-01
F 1 7 0. 0.
21 22 -1 0 1 0 0 2.643E+00 2.000E-01
F 1 7 0. 0.
21 23 -1 0 1 0 0 2.332E-01 2.000E-01
F 1 7 0. 0.
21 24 -1 0 1 0 0 7.083E-02 2.000E-01
F 1 7 0. 0.
21 25 -1 0 1 0 0 3.205E-02 2.000E-01
F 1 7 0. 0.
22 23 -1 0 1 0 0 3.369E+00 2.000E-01
F 1 7 0. 0.
22 24 -1 0 1 0 0 4.936E-01 2.000E-01
F 1 7 0. 0.
22 25 -1 0 1 0 0 1.688E-01 2.000E-01
F 1 7 0. 0.
23 24 -1 0 1 0 0 3.970E+00 2.000E-01
F 1 7 0. 0.
23 25 -1 0 1 0 0 5.729E-01 2.000E-01
F 1 7 0. 0.
24 25 -1 0 1 0 0 4.543E+00 2.000E-01
F 1 7 0. 0.
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+286
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****** Levels
2.36686693E+16 2. 2 'N V 2Se 1' 0 0. 0
2.12575067E+16 2. 2 'N V 2Po 1' 0 0. 0
2.12497511E+16 4. 2 'N V 2Po 1' 0 0. 0
9.99477544E+15 2. 3 'N V 2Se 2' 0 0. -104
9.34463014E+15 6. 3 'N V 2Po 2' 0 0. -104
9.14678677E+15 10. 3 'N V 2De 1' 0 0. -104
5.49155216E+15 2. 4 'N V 2Se 3' 0 0. -104
5.22728873E+15 6. 4 'N V 2Po 3' 0 0. -104
5.14458753E+15 10. 4 'N V 2De 2' 0 0. -104
5.13698758E+15 14. 4 'N V 2Fo 1' 0 0. -104
3.30411619E+15 50. 5 'N V +2__ 1' 0 0. -104
2.28994449E+15 72. 6 'N V +2__ 2' 0 0. -104
1.68078485E+15 98. 7 'N V +2__ 3' 0 0. -104
1.28615856E+15 128. 8 'N V +2__ 4' 0 0. -104
1.01594244E+15 162. 9 'N V +2__ 5' 0 0. -104
8.22729977E+14 200. 10 'N V +2__ 6' 0 0. -104
****** Continuum transitions
1 17 1 117 0 0 0 1.305E-19 0.000E+00
-0.0154 0.0105 0.1463 0.3403 0.5601 0.6765 0.6830 0.7218 0.7282 0.7412
0.7476 0.7605 0.8899 1.0257 1.2261 1.2778 1.4444
-0.3297 -0.3589 -0.6042 -0.9916 -1.4594 -1.7202 -1.7247 -0.8013 -0.6566 -0.5262
-0.5008 -0.5038 -0.8238 -1.1798 -1.7315 -1.8783 -2.3623
2 17 1 108 0 0 0 1.796E-19 0.000E+00
-0.0172 0.0022 0.0540 0.2480 0.4355 0.6230 0.8170 0.9044
-0.2081 -0.2403 -0.3869 -0.9799 -1.5861 -2.2206 -2.9096 -3.2349
3 17 1 108 0 0 0 1.796E-19 0.000E+00
-0.0172 0.0022 0.0540 0.2480 0.4355 0.6230 0.8170 0.9044
-0.2081 -0.2403 -0.3869 -0.9799 -1.5861 -2.2206 -2.9096 -3.2349
4 17 1 109 0 0 0 2.188E-19 0.000E+00
-0.0373 -0.0050 0.2149 0.4476 0.6998 0.9197 1.1589 1.3335 1.3747
-0.0772 -0.1159 -0.5190 -0.9799 -1.5144 -2.0090 -2.5806 -3.0213 -3.1276
5 17 1 109 0 0 0 3.287E-19 0.000E+00
-0.0400 -0.0142 0.1410 0.3285 0.5160 0.6971 0.8781 1.0075 1.0522
0.1121 0.0747 -0.2972 -0.7816 -1.3021 -1.8381 -2.4075 -2.8383 -2.9901
6 17 1 108 0 0 0 2.159E-19 0.000E+00
-0.0409 -0.0215 0.0173 0.1854 0.3535 0.5281 0.6897 0.7817
-0.0304 -0.0676 -0.1927 -0.7875 -1.4127 -2.0966 -2.7629 -3.1583
7 17 1 108 0 0 0 3.176E-19 0.000E+00
-0.0705 -0.0382 0.2140 0.5050 0.8089 1.0934 1.3650 1.4233
0.1430 0.1033 -0.3646 -0.9377 -1.5731 -2.1988 -2.8285 -2.9690
8 17 1 109 0 0 0 4.926E-19 0.000E+00
-0.0744 -0.0485 0.1067 0.3136 0.5011 0.6886 0.8567 1.0636 1.1426
0.3534 0.3181 -0.0198 -0.5027 -0.9716 -1.4714 -1.9488 -2.5670 -2.8164
9 17 1 110 0 0 0 4.314E-19 0.000E+00
-0.0757 -0.0498 0.0472 0.2089 0.3511 0.5063 0.6485 0.7973 0.8943 0.9135
0.3411 0.2964 0.0311 -0.4467 -0.8958 -1.4180 -1.9261 -2.4871 -2.8759 -2.9508
10 17 1 2 0 0 0 3.796E-19 0.000E+00
3.000 1.265 1.000 0.000
11 17 1 102 0 0 0 5.522E-20 0.000E+00
0.002 1.475
-0.739 -4.428
12 17 1 102 0 0 0 5.521E-20 0.000E+00
-0.002 1.493
-0.731 -4.454
13 17 1 102 0 0 0 5.521E-20 0.000E+00
-0.002 1.577
-0.731 -4.674
14 17 1 102 0 0 0 5.410E-20 0.000E+00
-0.002 1.684
-0.739 -4.965
15 17 1 102 0 0 0 5.633E-20 0.000E+00
-0.002 1.617
-0.722 -4.780
16 17 1 103 0 0 0 4.800E-20 0.000E+00
0.012 0.812 1.609
-0.827 -3.019 -4.947
*** Line transitions
1 2 -1 1 1 0 0 7.790E-02 7.000E-01
T 3 15 175. 0.
3.4E+8 4.4E-7 0. 0. 0.
1 3 -1 1 1 0 0 1.560E-01 7.000E-01
T 3 15 175. 0.
3.4E+8 4.4E-7 0. 0. 0.
1 4 0 0 4 0 0 0.000E+00 5.000E-02
1 5 -1 0 1 0 0 2.385E-01 2.000E-01
F 1 7 0. 0.
1 6 0 0 4 0 0 0.000E+00 5.000E-02
1 7 0 0 4 0 0 0.000E+00 5.000E-02
1 8 -1 0 1 0 0 6.850E-02 2.000E-01
F 1 7 0. 0.
1 9 0 0 4 0 0 0.000E+00 5.000E-02
1 10 0 0 4 0 0 0.000E+00 5.000E-02
1 11 -1 0 1 0 0 2.995E-02 2.000E-01
F 1 7 0. 0.
1 12 -1 0 1 0 0 1.590E-02 2.000E-01
F 1 7 0. 0.
1 13 -1 0 1 0 0 9.550E-03 2.000E-01
F 1 7 0. 0.
1 14 -1 0 1 0 0 6.200E-03 2.000E-01
F 1 7 0. 0.
1 15 -1 0 1 0 0 4.250E-03 2.000E-01
F 1 7 0. 0.
1 16 -1 0 1 0 0 3.050E-03 2.000E-01
F 1 7 0. 0.
2 3 0 0 4 0 0 0.000E+00 5.000E-02
2 4 -1 0 1 0 0 3.233E-02 2.000E-01
F 1 7 0. 0.
2 5 0 0 4 0 0 0.000E+00 5.000E-02
2 6 -1 0 1 0 0 6.517E-01 2.000E-01
F 1 7 0. 0.
2 7 -1 0 1 0 0 6.250E-03 2.000E-01
F 1 7 0. 0.
2 8 0 0 4 0 0 0.000E+00 5.000E-02
2 9 -1 0 1 0 0 1.225E-01 2.000E-01
F 1 7 0. 0.
2 10 0 0 4 0 0 0.000E+00 5.000E-02
2 11 -1 0 1 0 0 4.805E-02 2.000E-01
F 1 7 0. 0.
2 12 -1 0 1 0 0 2.369E-02 2.000E-01
F 1 7 0. 0.
2 13 -1 0 1 0 0 1.364E-02 2.000E-01
F 1 7 0. 0.
2 14 -1 0 1 0 0 8.602E-03 2.000E-01
F 1 7 0. 0.
2 15 -1 0 1 0 0 5.810E-03 2.000E-01
F 1 7 0. 0.
2 16 -1 0 1 0 0 4.125E-03 2.000E-01
F 1 7 0. 0.
3 4 -1 0 1 0 0 3.233E-02 2.000E-01
F 1 7 0. 0.
3 5 0 0 4 0 0 0.000E+00 5.000E-02
3 6 -1 0 1 0 0 6.517E-01 2.000E-01
F 1 7 0. 0.
3 7 -1 0 1 0 0 6.250E-03 2.000E-01
F 1 7 0. 0.
3 8 0 0 4 0 0 0.000E+00 5.000E-02
3 9 -1 0 1 0 0 1.225E-01 2.000E-01
F 1 7 0. 0.
3 10 0 0 4 0 0 0.000E+00 5.000E-02
3 11 -1 0 1 0 0 4.805E-02 2.000E-01
F 1 7 0. 0.
3 12 -1 0 1 0 0 2.369E-02 2.000E-01
F 1 7 0. 0.
3 13 -1 0 1 0 0 1.364E-02 2.000E-01
F 1 7 0. 0.
3 14 -1 0 1 0 0 8.602E-03 2.000E-01
F 1 7 0. 0.
3 15 -1 0 1 0 0 5.810E-03 2.000E-01
F 1 7 0. 0.
3 16 -1 0 1 0 0 4.125E-03 2.000E-01
F 1 7 0. 0.
4 5 -1 0 1 0 0 3.940E-01 7.000E-01
F 1 7 0. 0.
4 6 0 0 4 0 0 0.000E+00 5.000E-02
4 7 0 0 4 0 0 0.000E+00 5.000E-02
4 8 -1 0 1 0 0 2.455E-01 2.000E-01
F 1 7 0. 0.
4 9 0 0 4 0 0 0.000E+00 5.000E-02
4 10 0 0 4 0 0 0.000E+00 5.000E-02
4 11 -1 0 1 0 0 7.550E-02 2.000E-01
F 1 7 0. 0.
4 12 -1 0 1 0 0 3.435E-02 2.000E-01
F 1 7 0. 0.
4 13 -1 0 1 0 0 1.895E-02 2.000E-01
F 1 7 0. 0.
4 14 -1 0 1 0 0 1.170E-02 2.000E-01
F 1 7 0. 0.
4 15 -1 0 1 0 0 7.800E-03 2.000E-01
F 1 7 0. 0.
4 16 -1 0 1 0 0 5.450E-03 2.000E-01
F 1 7 0. 0.
5 6 -1 0 1 0 0 5.333E-02 7.000E-01
F 1 7 0. 0.
5 7 -1 0 1 0 0 7.083E-02 2.000E-01
F 1 7 0. 0.
5 8 0 0 4 0 0 0.000E+00 5.000E-02
5 9 -1 0 1 0 0 5.483E-01 2.000E-01
F 1 7 0. 0.
5 10 0 0 4 0 0 0.000E+00 5.000E-02
5 11 -1 0 1 0 0 1.470E-01 2.000E-01
F 1 7 0. 0.
5 12 -1 0 1 0 0 6.047E-02 2.000E-01
F 1 7 0. 0.
5 13 -1 0 1 0 0 3.162E-02 2.000E-01
F 1 7 0. 0.
5 14 -1 0 1 0 0 1.881E-02 2.000E-01
F 1 7 0. 0.
5 15 -1 0 1 0 0 1.228E-02 2.000E-01
F 1 7 0. 0.
5 16 -1 0 1 0 0 8.493E-03 2.000E-01
F 1 7 0. 0.
6 7 0 0 4 0 0 0.000E+00 5.000E-02
6 8 -1 0 1 0 0 1.590E-02 2.000E-01
F 1 7 0. 0.
6 9 0 0 4 0 0 0.000E+00 5.000E-02
6 10 -1 0 1 0 0 1.097E+00 2.000E-01
F 1 7 0. 0.
6 11 -1 0 1 0 0 1.825E-01 2.000E-01
F 1 7 0. 0.
6 12 -1 0 1 0 0 6.570E-02 2.000E-01
F 1 7 0. 0.
6 13 -1 0 1 0 0 3.210E-02 2.000E-01
F 1 7 0. 0.
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F 1 7 0. 0.
6 15 -1 0 1 0 0 1.170E-02 2.000E-01
F 1 7 0. 0.
6 16 -1 0 1 0 0 7.951E-03 2.000E-01
F 1 7 0. 0.
7 8 -1 0 1 0 0 5.400E-01 7.000E-01
F 1 7 0. 0.
7 9 0 0 4 0 0 0.000E+00 5.000E-02
7 10 0 0 4 0 0 0.000E+00 5.000E-02
7 11 -1 0 1 0 0 2.630E-01 2.000E-01
F 1 7 0. 0.
7 12 -1 0 1 0 0 8.200E-02 2.000E-01
F 1 7 0. 0.
7 13 -1 0 1 0 0 3.825E-02 2.000E-01
F 1 7 0. 0.
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F 1 7 0. 0.
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F 1 7 0. 0.
7 16 -1 0 1 0 0 9.100E-03 2.000E-01
F 1 7 0. 0.
8 9 -1 0 1 0 0 9.500E-02 7.000E-01
F 1 7 0. 0.
8 10 0 0 4 0 0 0.000E+00 5.000E-02
8 11 -1 0 1 0 0 6.367E-01 2.000E-01
F 1 7 0. 0.
8 12 -1 0 1 0 0 1.597E-01 2.000E-01
F 1 7 0. 0.
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F 1 7 0. 0.
8 14 -1 0 1 0 0 3.670E-02 2.000E-01
F 1 7 0. 0.
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F 1 7 0. 0.
8 16 -1 0 1 0 0 1.480E-02 2.000E-01
F 1 7 0. 0.
9 10 0 0 4 0 0 0.000E+00 5.000E-02
9 11 -1 0 1 0 0 1.383E+00 2.000E-01
F 1 7 0. 0.
9 12 -1 0 1 0 0 2.195E-01 2.000E-01
F 1 7 0. 0.
9 13 -1 0 1 0 0 7.786E-02 2.000E-01
F 1 7 0. 0.
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F 1 7 0. 0.
9 15 -1 0 1 0 0 2.171E-02 2.000E-01
F 1 7 0. 0.
9 16 -1 0 1 0 0 1.381E-02 2.000E-01
F 1 7 0. 0.
10 11 -1 0 1 0 0 2.689E+00 2.000E-01
F 1 7 0. 0.
10 12 -1 0 1 0 0 4.234E-01 2.000E-01
F 1 7 0. 0.
10 13 -1 0 1 0 0 1.497E-01 2.000E-01
F 1 7 0. 0.
10 14 -1 0 1 0 0 7.260E-02 2.000E-01
F 1 7 0. 0.
10 15 -1 0 1 0 0 4.163E-02 2.000E-01
F 1 7 0. 0.
10 16 -1 0 1 0 0 2.646E-02 2.000E-01
F 1 7 0. 0.
11 12 -1 0 1 0 0 2.460E+00 2.000E-01
F 1 7 0. 0.
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F 1 7 0. 0.
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F 1 7 0. 0.
11 15 -1 0 1 0 0 6.661E-02 2.000E-01
F 1 7 0. 0.
11 16 -1 0 1 0 0 3.834E-02 2.000E-01
F 1 7 0. 0.
12 13 -1 0 1 0 0 3.093E+00 2.000E-01
F 1 7 0. 0.
12 14 -1 0 1 0 0 4.707E-01 2.000E-01
F 1 7 0. 0.
12 15 -1 0 1 0 0 1.634E-01 2.000E-01
F 1 7 0. 0.
12 16 -1 0 1 0 0 7.854E-02 2.000E-01
F 1 7 0. 0.
13 14 -1 0 1 0 0 3.680E+00 2.000E-01
F 1 7 0. 0.
13 15 -1 0 1 0 0 5.468E-01 2.000E-01
F 1 7 0. 0.
13 16 -1 0 1 0 0 1.869E-01 2.000E-01
F 1 7 0. 0.
14 15 -1 0 1 0 0 4.240E+00 2.000E-01
F 1 7 0. 0.
14 16 -1 0 1 0 0 6.186E-01 2.000E-01
F 1 7 0. 0.
15 16 -1 0 1 0 0 4.783E+00 2.000E-01
F 1 7 0. 0.
+981
View File
@@ -0,0 +1,981 @@
****** Levels
5.21412627E+15 1. 2 'Ne I 1Se 1' 0 0. 0
1.19107791E+15 9. 3 'Ne I 3Po 1' 0 0. 0
1.14842634E+15 3. 3 'Ne I 1Po 1' 0 0. 0
7.49665335E+14 3. 3 'Ne I 3Se 1' 0 0. -104
7.25564864E+14 15. 3 'Ne I 3De 1' 0 0. -104
7.10086675E+14 9. 3 'Ne I 3Pe 1' 0 0. -104
7.00996846E+14 5. 3 'Ne I 1De 1' 0 0. -104
6.92605017E+14 3. 3 'Ne I 1Pe 1' 0 0. -104
6.71757715E+14 1. 3 'Ne I 1Se 2' 0 0. -104
4.57331607E+14 9. 4 'Ne I 3Po 2' 0 0. -104
4.32698024E+14 3. 4 'Ne I 1Po 2' 0 0. -104
3.72005036E+14 3. 4 'Ne I 1Po 3' 0 0. -104
3.69886811E+14 21. 4 'Ne I 3Fo 1' 0 0. -104
3.69074089E+14 9. 4 'Ne I 3Po 3' 0 0. -104
3.66603611E+14 7. 4 'Ne I 1Fo 1' 0 0. -104
3.45351609E+14 15. 4 'Ne I 3Do 1' 0 0. -104
3.44864902E+14 5. 4 'Ne I 1Do 1' 0 0. -104
3.35485600E+14 3. 4 'Ne I 3Se 2' 0 0. -104
3.31873599E+14 15. 4 'Ne I 3De 2' 0 0. -104
3.26791177E+14 9. 4 'Ne I 3Pe 2' 0 0. -104
3.24597992E+14 5. 4 'Ne I 1De 2' 0 0. -104
3.06985640E+14 3. 4 'Ne I 1Pe 2' 0 0. -104
3.02102329E+14 1. 4 'Ne I 1Se 3' 0 0. -104
2.06016948E+14 144. 5 'Ne I+3__ 1' 0 0. -104
1.89720416E+14 48. 5 'Ne I+1__ 2' 0 0. -104
1.31527871E+14 192. 6 'Ne I+3__ 3' 0 0. -104
1.23151954E+14 64. 6 'Ne I+1__ 4' 0 0. -104
9.12099975E+13 219. 7 'Ne I+3__ 5' 0 0. -104
9.10254397E+13 73. 7 'Ne I+1__ 6' 0 0. -104
6.70167403E+13 219. 8 'Ne I+3__ 7' 0 0. -104
6.68996353E+13 73. 8 'Ne I+1__ 8' 0 0. -104
5.13160470E+13 219. 9 'Ne I+3__ 9' 0 0. -104
5.12378190E+13 73. 9 'Ne I+1__10' 0 0. -104
3.70712175E+13 411. 10 'Ne I+3__11' 0 0. -104
3.70323363E+13 137. 10 'Ne I+1__12' 0 0. -104
****** Continuum transitions
1 36 1 107 0 0 0 6.0026E-19 0.0000E+00
0.0043 0.0576 0.1409 0.2263 0.3395 0.3801 1.0484
0.7862 0.8845 0.9569 0.9672 0.9414 0.9103 -1.0966
2 36 1 110 0 0 0 8.9822E-21 0.0000E+00
0.0018 0.0516 0.2224 0.3292 0.6672 0.7313 0.7527 0.7776 0.8345 1.4929
-1.0518 -1.1966 -0.8345 -0.7931 -0.9690 -0.8345 0.0862 -1.2483 -1.3414 -3.3173
3 36 1 109 0 0 0 2.7610E-20 0.0000E+00
-0.0018 0.0827 0.3452 0.6877 0.7366 0.7678 0.7989 0.8390 1.5151
-0.5552 -0.7311 -0.7931 -1.1035 -1.0311 0.4379 -1.1242 -1.3000 -3.3173
4 36 1 107 0 0 0 9.9965E-19 0.0000E+00
-0.0018 0.3585 0.4875 0.6254 0.9635 1.0347 1.6886
1.0069 -0.4000 -0.8000 -0.9242 -1.0621 -1.2138 -3.1863
5 36 1 106 0 0 0 6.9044E-19 0.0000E+00
0.0027 0.3630 0.4786 0.9591 1.0035 1.6841
0.8275 -0.7449 -0.9518 -1.1311 -1.2414 -3.2552
6 36 1 108 0 0 0 5.1930E-19 0.0000E+00
0.0027 0.3318 0.4030 0.4920 0.7589 1.0035 1.0658 1.7064
0.7034 -0.7863 -0.9656 -1.0345 -1.0759 -1.2414 -1.3656 -3.2828
7 36 1 107 0 0 0 6.3290E-19 0.0000E+00
-0.0062 0.3185 0.4164 0.9546 0.9813 1.0035 1.7153
0.8275 -0.5362 -0.8380 -1.2000 -0.5000 -1.2242 -3.2880
8 36 1 108 0 0 0 6.3980E-19 0.0000E+00
-0.0018 0.3674 0.4875 0.9279 0.9813 1.0035 1.0347 1.7153
0.8137 -0.7725 -1.0207 -1.1863 -0.8690 -1.4207 -1.4207 -3.4483
9 36 1 111 0 0 0 1.1085E-19 0.0000E+00
-0.0018 0.0783 0.1628 0.3318 0.4164 0.6521 0.9413 0.9946 1.0035 1.0302
1.7197
0.0517 -0.2587 -0.3207 -0.2587 -0.2793 -0.4449 -0.7242 -0.2690 -1.1173 -0.9000
-2.9173
10 36 1 112 0 0 0 6.0097E-20 0.0000E+00
0.0027 0.1450 0.2562 0.4564 0.5587 0.7455 1.0658 1.1192 1.1370 1.1681
1.1904 1.8487
-0.2345 -0.9518 -1.1035 -1.0207 -1.0345 -1.1725 -1.5035 -1.5311 -1.3794 -0.4828
-1.7931 -3.7794
11 36 1 108 0 0 0 9.8523E-20 0.0000E+00
-0.0018 0.1717 0.2651 0.7277 1.1459 1.1948 1.2126 1.8532
-0.0000 -0.6207 -0.8000 -1.1725 -1.6966 -0.4414 -1.5725 -3.5311
12 36 1 112 0 0 0 1.6482E-18 0.0000E+00
0.0027 0.6966 0.7589 0.7900 0.8701 0.9502 1.1681 1.2260 1.2349 1.2571
1.2793 1.8487
1.2068 -1.4483 -1.2932 -0.2242 -2.1552 -2.4656 -2.7932 -2.7242 -2.3794 -1.0863
-3.2242 -4.9828
13 36 1 106 0 0 0 1.8547E-18 0.0000E+00
0.0027 1.1726 1.2349 1.2571 1.2971 1.8710
1.2586 -3.0173 -2.9483 -1.1897 -3.0518 -4.7932
14 36 1 107 0 0 0 1.7872E-18 0.0000E+00
-0.0018 0.6076 1.1325 1.2349 1.2616 1.2927 1.8799
1.2586 -0.9138 -2.8966 -3.5173 -1.2414 -2.6380 -4.4138
15 36 1 108 0 0 0 1.7867E-18 0.0000E+00
-0.0018 0.3585 1.1904 1.2304 1.2660 1.2882 1.3594 1.8621
1.2586 -0.0518 -3.1207 -2.8276 -1.5173 -3.1552 -3.3104 -4.8276
16 36 1 109 0 0 0 2.0949E-18 0.0000E+00
-0.0018 0.4208 0.9101 1.1503 1.2438 1.2660 1.2927 1.3194 1.8977
1.3275 -0.1725 -2.1380 -3.0690 -3.2759 -2.7587 -1.2932 -3.0173 -4.7587
17 36 1 111 0 0 0 2.0871E-18 0.0000E+00
0.0027 0.3096 0.7900 0.8256 0.8701 1.0124 1.2082 1.2571 1.2882 1.3105
1.8932
1.3103 0.2413 -1.6207 -1.0690 -1.8966 -2.5173 -3.0001 -2.7587 -1.9138 -3.0863
-4.8449
18 36 1 108 0 0 0 2.3657E-18 0.0000E+00
0.0027 0.2918 0.6121 0.7722 0.9012 1.2704 1.3372 1.9733
1.3655 0.4413 -0.6759 -1.1173 -1.2966 -1.5173 -1.6000 -3.5173
19 36 1 106 0 0 0 1.6667E-18 0.0000E+00
0.0071 0.1993 0.6477 0.7918 1.3149 2.0089
1.2000 0.6069 -1.0621 -1.2828 -1.6000 -3.7242
20 36 1 108 0 0 0 1.4329E-18 0.0000E+00
0.0071 0.2206 0.6050 0.7277 1.1922 1.3256 1.3416 2.0142
1.1310 0.3724 -1.1173 -1.3104 -1.5725 -1.7380 -1.6414 -3.6552
21 36 1 107 0 0 0 1.6279E-18 0.0000E+00
0.0071 0.5996 0.7598 1.2936 1.3203 1.3363 2.0142
1.1862 -0.9380 -1.2276 -1.6552 -0.6759 -1.6966 -3.6552
22 36 1 107 0 0 0 1.7873E-18 0.0000E+00
0.0071 0.7064 0.8505 1.2989 1.3416 1.3576 2.0302
1.2275 -1.2000 -1.3656 -1.6276 -1.0897 -1.8621 -3.8621
23 36 1 108 0 0 0 4.3734E-19 0.0000E+00
-0.0018 0.2117 0.3452 0.6032 0.8790 1.2749 1.3772 1.9644
0.6482 -0.2345 -0.5242 -0.5794 -0.7587 -1.2000 -1.2414 -3.0621
24 36 1 109 0 0 0 1.6388E-19 0.0000E+00
0.0071 0.2900 0.7064 0.9413 1.1281 1.4697 1.5124 1.5445 2.2064
0.1931 -0.6621 -2.1104 -2.8000 -3.1173 -3.4621 -2.3449 -3.5173 -5.5173
25 36 1 112 0 0 0 5.4150E-19 0.0000E+00
-0.0036 0.3007 0.6477 0.9092 1.0320 1.0480 1.1014 1.4804 1.5338 1.5498
1.5765 2.2331
0.7448 -0.2069 -1.4207 -2.1518 -2.3035 -1.9587 -2.4414 -2.8828 -2.7863 -2.4690
-2.9104 -4.8414
26 36 1 111 0 0 0 2.0923E-19 0.0000E+00
-0.0036 0.3434 0.9626 1.1121 1.2349 1.3897 1.6566 1.6939 1.7099 1.7420
2.3772
0.3310 -0.6759 -2.6897 -3.1035 -3.3931 -3.6138 -3.8621 -3.6690 -3.1311 -3.8897
-5.7931
27 36 1 112 0 0 0 6.5338E-19 0.0000E+00
0.0018 0.2633 1.0534 1.1922 1.2242 1.2722 1.4911 1.6886 1.7313 1.7420
1.7687 2.3559
0.8103 0.0862 -2.4138 -2.6207 -2.3794 -2.8104 -3.1035 -3.2587 -3.0863 -2.2587
-3.2414 -5.0001
28 36 1 110 0 0 0 2.6665E-19 0.0000E+00
-0.0018 0.5400 1.0507 1.2873 1.4430 1.8229 1.8541 1.8603 1.8914 2.4955
0.4310 -1.0863 -2.7759 -3.4483 -3.7587 -4.1552 -3.6380 -3.0690 -4.1552 -5.9311
29 36 1 111 0 0 0 7.1119E-19 0.0000E+00
-0.0036 0.4021 1.1655 1.3256 1.3470 1.3897 1.8060 1.8541 1.8648 1.8808
2.4092
0.8620 -0.2759 -2.6380 -2.8794 -2.6207 -3.0690 -3.5690 -3.3449 -1.9656 -3.4311
-4.9828
30 36 1 109 0 0 0 3.8122E-19 0.0000E+00
0.0044 0.6210 1.2188 1.4119 1.5801 1.9662 1.9973 2.0160 2.5765
0.5689 -1.1380 -3.0518 -3.6035 -3.9656 -4.3449 -3.1207 -4.2932 -5.9656
31 36 1 111 0 0 0 1.0852E-18 0.0000E+00
0.0124 0.5249 1.2615 1.4484 1.4804 1.5178 1.9502 1.9875 2.0035 2.0196
2.4733
0.9999 -0.4656 -2.7414 -3.0690 -2.8276 -3.2587 -3.7759 -3.5518 -2.3794 -3.5518
-4.8966
32 36 1 110 0 0 0 4.8748E-19 0.0000E+00
0.0044 0.3719 0.8701 1.5053 1.6735 2.0534 2.1032 2.1219 2.1343 2.6512
0.6758 -0.3311 -1.7518 -3.7380 -4.0690 -4.5242 -4.2621 -3.6276 -4.4552 -5.9587
33 36 1 111 0 0 0 1.4130E-18 0.0000E+00
0.0044 0.5898 1.2749 1.5302 1.5863 1.6236 2.0658 2.0970 2.1156 2.1343
2.5080
1.1379 -0.4828 -2.6380 -3.2242 -3.0001 -3.3794 -3.9311 -3.6725 -2.4483 -3.7070
-4.8276
34 36 1 113 0 0 0 1.4564E-19 0.0000E+00
-0.0080 0.0356 0.0418 0.4777 1.0196 1.5302 1.7295 1.8790 2.2153 2.2464
2.2589 2.2713 2.7260
0.1379 0.2758 0.5862 -0.5518 -2.1035 -3.7414 -4.2242 -4.5001 -4.8794 -4.5345
-3.8621 -4.7932 -6.1207
35 36 1 113 0 0 0 4.2424E-19 0.0000E+00
-0.0018 0.0293 0.0480 0.6646 1.5365 1.7046 1.7295 1.7607 2.2091 2.2340
2.2589 2.2776 2.6139
0.6206 0.7413 1.0689 -0.6552 -3.2587 -3.5690 -3.3621 -3.7414 -4.3104 -4.0173
-3.1207 -4.0345 -5.0173
*** Line transitions
1 2 0 0 4 0 0 0.000E+00 5.000E-02
1 3 -1 0 1 0 0 1.700E-01 2.000E-01
F 1 7 0. 0.
1 4 0 0 4 0 0 0.000E+00 5.000E-02
1 5 0 0 4 0 0 0.000E+00 5.000E-02
1 6 0 0 4 0 0 0.000E+00 5.000E-02
1 7 0 0 4 0 0 0.000E+00 5.000E-02
1 8 0 0 4 0 0 0.000E+00 5.000E-02
1 9 0 0 4 0 0 0.000E+00 5.000E-02
1 10 0 0 4 0 0 0.000E+00 5.000E-02
1 11 -1 0 1 0 0 3.480E-02 2.000E-01
F 1 7 0. 0.
1 12 -1 0 1 0 0 2.310E-02 2.000E-01
F 1 7 0. 0.
1 13 0 0 4 0 0 0.000E+00 5.000E-02
1 14 0 0 4 0 0 0.000E+00 5.000E-02
1 15 0 0 4 0 0 0.000E+00 5.000E-02
1 16 0 0 4 0 0 0.000E+00 5.000E-02
1 17 0 0 4 0 0 0.000E+00 5.000E-02
1 18 0 0 4 0 0 0.000E+00 5.000E-02
1 19 0 0 4 0 0 0.000E+00 5.000E-02
1 20 0 0 4 0 0 0.000E+00 5.000E-02
1 21 0 0 4 0 0 0.000E+00 5.000E-02
1 22 0 0 4 0 0 0.000E+00 5.000E-02
1 23 0 0 4 0 0 0.000E+00 5.000E-02
1 24 0 0 4 0 0 0.000E+00 5.000E-02
1 25 -1 0 1 0 0 2.520E-02 2.000E-01
F 1 7 0. 0.
1 26 0 0 4 0 0 0.000E+00 5.000E-02
1 27 -1 0 1 0 0 1.309E-02 2.000E-01
F 1 7 0. 0.
1 28 0 0 4 0 0 0.000E+00 5.000E-02
1 29 -1 0 1 0 0 7.610E-03 2.000E-01
F 1 7 0. 0.
1 30 0 0 4 0 0 0.000E+00 5.000E-02
1 31 -1 0 1 0 0 4.800E-03 2.000E-01
F 1 7 0. 0.
1 32 0 0 4 0 0 0.000E+00 5.000E-02
1 33 -1 0 1 0 0 3.210E-03 2.000E-01
F 1 7 0. 0.
1 34 0 0 4 0 0 0.000E+00 5.000E-02
1 35 -1 0 1 0 0 3.903E-03 2.000E-01
F 1 7 0. 0.
2 3 0 0 4 0 0 0.000E+00 5.000E-02
2 4 -1 0 1 0 0 1.047E-01 7.000E-01
F 1 7 0. 0.
2 5 -1 0 1 0 0 5.489E-01 7.000E-01
F 1 7 0. 0.
2 6 -1 0 1 0 0 3.311E-01 7.000E-01
F 1 7 0. 0.
2 7 0 0 4 0 0 0.000E+00 5.000E-02
2 8 0 0 4 0 0 0.000E+00 5.000E-02
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2 12 0 0 4 0 0 0.000E+00 5.000E-02
2 13 0 0 4 0 0 0.000E+00 5.000E-02
2 14 0 0 4 0 0 0.000E+00 5.000E-02
2 15 0 0 4 0 0 0.000E+00 5.000E-02
2 16 0 0 4 0 0 0.000E+00 5.000E-02
2 17 0 0 4 0 0 0.000E+00 5.000E-02
2 18 -1 0 1 0 0 4.622E-05 2.000E-01
F 1 7 0. 0.
2 19 -1 0 1 0 0 4.622E-03 2.000E-01
F 1 7 0. 0.
2 20 -1 0 1 0 0 5.289E-03 2.000E-01
F 1 7 0. 0.
2 21 0 0 4 0 0 0.000E+00 5.000E-02
2 22 0 0 4 0 0 0.000E+00 5.000E-02
2 23 0 0 4 0 0 0.000E+00 5.000E-02
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F 1 7 0. 0.
2 25 0 0 4 0 0 0.000E+00 5.000E-02
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F 1 7 0. 0.
2 27 0 0 4 0 0 0.000E+00 5.000E-02
2 28 -1 0 1 0 0 1.908E-04 2.000E-01
F 1 7 0. 0.
2 29 0 0 4 0 0 0.000E+00 5.000E-02
2 30 -1 0 1 0 0 1.028E-04 2.000E-01
F 1 7 0. 0.
2 31 0 0 4 0 0 0.000E+00 5.000E-02
2 32 -1 0 1 0 0 6.252E-05 2.000E-01
F 1 7 0. 0.
2 33 0 0 4 0 0 0.000E+00 5.000E-02
2 34 -1 0 1 0 0 4.242E-05 2.000E-01
F 1 7 0. 0.
2 35 0 0 4 0 0 0.000E+00 5.000E-02
3 4 0 0 4 0 0 0.000E+00 5.000E-02
3 5 0 0 4 0 0 0.000E+00 5.000E-02
3 6 0 0 4 0 0 0.000E+00 5.000E-02
3 7 -1 0 1 0 0 5.500E-01 7.000E-01
F 1 7 0. 0.
3 8 -1 0 1 0 0 3.280E-01 7.000E-01
F 1 7 0. 0.
3 9 -1 0 1 0 0 1.253E-01 2.000E-01
F 1 7 0. 0.
3 10 0 0 4 0 0 0.000E+00 5.000E-02
3 11 0 0 4 0 0 0.000E+00 5.000E-02
3 12 0 0 4 0 0 0.000E+00 5.000E-02
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3 14 0 0 4 0 0 0.000E+00 5.000E-02
3 15 0 0 4 0 0 0.000E+00 5.000E-02
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3 17 0 0 4 0 0 0.000E+00 5.000E-02
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F 1 7 0. 0.
3 22 -1 0 1 0 0 2.683E-03 2.000E-01
F 1 7 0. 0.
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F 1 7 0. 0.
3 24 0 0 4 0 0 0.000E+00 5.000E-02
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F 1 7 0. 0.
3 26 0 0 4 0 0 0.000E+00 5.000E-02
3 27 -1 0 1 0 0 8.603E-04 2.000E-01
F 1 7 0. 0.
3 28 0 0 4 0 0 0.000E+00 5.000E-02
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F 1 7 0. 0.
3 30 0 0 4 0 0 0.000E+00 5.000E-02
3 31 -1 0 1 0 0 2.505E-04 2.000E-01
F 1 7 0. 0.
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F 1 7 0. 0.
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3 35 -1 0 1 0 0 1.099E-04 2.000E-01
F 1 7 0. 0.
4 5 0 0 4 0 0 0.000E+00 5.000E-02
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4 7 0 0 4 0 0 0.000E+00 5.000E-02
4 8 0 0 4 0 0 0.000E+00 5.000E-02
4 9 0 0 4 0 0 0.000E+00 5.000E-02
4 10 -1 0 1 0 0 1.120E-01 2.000E-01
F 1 7 0. 0.
4 11 0 0 4 0 0 0.000E+00 5.000E-02
4 12 0 0 4 0 0 0.000E+00 5.000E-02
4 13 0 0 4 0 0 0.000E+00 5.000E-02
4 14 -1 0 1 0 0 8.567E-01 2.000E-01
F 1 7 0. 0.
4 15 0 0 4 0 0 0.000E+00 5.000E-02
4 16 0 0 4 0 0 0.000E+00 5.000E-02
4 17 0 0 4 0 0 0.000E+00 5.000E-02
4 18 0 0 4 0 0 0.000E+00 5.000E-02
4 19 0 0 4 0 0 0.000E+00 5.000E-02
4 20 0 0 4 0 0 0.000E+00 5.000E-02
4 21 0 0 4 0 0 0.000E+00 5.000E-02
4 22 0 0 4 0 0 0.000E+00 5.000E-02
4 23 0 0 4 0 0 0.000E+00 5.000E-02
4 24 -1 0 1 0 0 1.234E-01 2.000E-01
F 1 7 0. 0.
4 25 0 0 4 0 0 0.000E+00 5.000E-02
4 26 -1 0 1 0 0 4.023E-02 2.000E-01
F 1 7 0. 0.
4 27 0 0 4 0 0 0.000E+00 5.000E-02
4 28 -1 0 1 0 0 1.847E-02 2.000E-01
F 1 7 0. 0.
4 29 0 0 4 0 0 0.000E+00 5.000E-02
4 30 -1 0 1 0 0 1.017E-02 2.000E-01
F 1 7 0. 0.
4 31 0 0 4 0 0 0.000E+00 5.000E-02
4 32 -1 0 1 0 0 6.270E-03 2.000E-01
F 1 7 0. 0.
4 33 0 0 4 0 0 0.000E+00 5.000E-02
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F 1 7 0. 0.
4 35 0 0 4 0 0 0.000E+00 5.000E-02
5 6 0 0 4 0 0 0.000E+00 5.000E-02
5 7 0 0 4 0 0 0.000E+00 5.000E-02
5 8 0 0 4 0 0 0.000E+00 5.000E-02
5 9 0 0 4 0 0 0.000E+00 5.000E-02
5 10 -1 0 1 0 0 1.627E-01 2.000E-01
F 1 7 0. 0.
5 11 0 0 4 0 0 0.000E+00 5.000E-02
5 12 0 0 4 0 0 0.000E+00 5.000E-02
5 13 -1 0 1 0 0 7.467E-01 2.000E-01
F 1 7 0. 0.
5 14 -1 0 1 0 0 1.187E-02 2.000E-01
F 1 7 0. 0.
5 15 0 0 4 0 0 0.000E+00 5.000E-02
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F 1 7 0. 0.
5 17 0 0 4 0 0 0.000E+00 5.000E-02
5 18 0 0 4 0 0 0.000E+00 5.000E-02
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5 24 -1 0 1 0 0 1.080E-01 2.000E-01
F 1 7 0. 0.
5 25 0 0 4 0 0 0.000E+00 5.000E-02
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F 1 7 0. 0.
5 27 0 0 4 0 0 0.000E+00 5.000E-02
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F 1 7 0. 0.
5 29 0 0 4 0 0 0.000E+00 5.000E-02
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F 1 7 0. 0.
5 31 0 0 4 0 0 0.000E+00 5.000E-02
5 32 -1 0 1 0 0 4.773E-03 2.000E-01
F 1 7 0. 0.
5 33 0 0 4 0 0 0.000E+00 5.000E-02
5 34 -1 0 1 0 0 5.318E-03 2.000E-01
F 1 7 0. 0.
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-0.0029 0.0100 0.0294 0.1070 0.2169 0.8825
0.6330 0.6024 0.5482 0.4144 0.1718 -1.8245
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0.2232 0.4107 0.8920
0.5785 0.6054 0.6085 0.5720 0.6280 0.6292 0.6048 0.5228 0.4888 0.4486
0.2068 -0.3505 -1.7970
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0.8973
0.4983 0.5922 0.6082 0.6120 0.6023 0.5254 0.5082 0.4796 0.2510 0.1468
-1.7812
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0.0997 0.1061 0.1126 0.1191 0.1255 0.1320 0.1384 0.1643 0.1966 0.2290
0.2678 0.9309
1.0660 1.0366 0.9757 0.7868 0.7335 0.7451 0.8984 0.9200 0.9455 1.0182
1.0197 0.9711 0.8813 0.7766 0.6917 0.6390 0.6103 0.5704 0.4979 0.4368
0.3466 -1.6428
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0.1573 0.1703 0.1897 0.2026 0.2866 0.4030 0.9568
0.8041 0.7850 0.7240 0.5371 0.5519 0.6879 0.8380 0.9299 0.9485 0.9089
0.7654 0.7033 0.6742 0.7001 0.8258 0.8548 0.8499 0.8211 0.6877 0.6539
0.6334 0.6191 0.6174 0.5956 0.4123 0.0690 -1.5948
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0.0599 0.0664 0.0728 0.0793 0.0858 0.0922 0.0987 0.1052 0.1116 0.1181
0.1246 0.1375 0.1440 0.1504 0.1698 0.1763 0.1828 0.2022 0.2474 0.2927
0.3315 0.9769
1.3386 1.4285 1.4601 1.4220 1.3047 1.1028 0.8289 0.5342 0.3444 0.3818
0.5631 0.7671 0.9238 1.0037 0.9930 0.8969 0.7357 0.5617 0.4575 0.4546
0.5067 0.6343 0.6781 0.7005 0.7262 0.7257 0.7113 0.6318 0.5723 0.4869
0.3853 -1.5532
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0.0597 0.0662 0.0726 0.0791 0.0856 0.0920 0.0985 0.1050 0.1114 0.1244
0.1308 0.1373 0.1567 0.1632 0.1696 0.1826 0.1955 0.2084 0.2278 0.2666
0.3183 0.4606 0.9868
0.4223 0.4547 0.4424 0.3768 0.2666 0.1757 0.2716 0.5396 0.8270 1.0434
1.1726 1.2203 1.1998 1.1269 1.0149 0.8718 0.7157 0.6075 0.6246 0.8305
0.8762 0.8676 0.7371 0.7099 0.6955 0.6946 0.7014 0.6855 0.6358 0.5787
0.4716 0.0504 -1.5308
8 13 1 115 0 0 0 1.760E-19 0.000E+00
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0.2640 0.3868 0.4256 0.4903 1.0911
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0.0570 0.0635 0.0699 0.0828 0.0893 0.0958 0.1022 0.1087 0.1152 0.1281
0.1346 0.1410 0.1475 0.1540 0.1604 0.1669 0.1734 0.1798 0.1928 0.1992
0.2057 0.2186 0.2251 0.2316 0.2380 0.2445 0.2510 0.2574 0.2639 0.2704
0.2768 0.2833 0.2898 0.2962 0.3027 0.3092 0.3156 0.3286 0.3350 0.3544
0.3674 0.4191 0.4579 1.0944
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0.0560 0.1364 0.2075 0.2610 0.3004 0.3229 0.3171 0.2750 0.1397 0.1644
0.3235 0.8123 1.0067 1.1448 1.2296 1.2626 1.2382 1.1489 0.9934 0.7920
0.6195 0.5908 0.6884 0.7965 0.8595 0.8728 0.8513 0.7832 0.7659 0.7719
0.7555 0.6706 0.5663 -1.3455
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****** Levels
1.75624563E+16 1. 3 'S V 1Se 1' 0 0. 0
1.50496180E+16 9. 3 'S V 3Po 1' 0 0. 0
1.37485747E+16 3. 3 'S V 1Po 1' 0 0. 0
1.17512796E+16 5. 3 'S V 1De 1' 0 0. 0
1.15407661E+16 9. 3 'S V 3Pe 1' 0 0. 0
1.05151429E+16 15. 3 'S V 3De 1' 0 0. 0
1.05031686E+16 1. 3 'S V 1Se 2' 0 0. -105
9.44283671E+15 5. 3 'S V 1De 2' 0 0. -105
8.21617419E+15 3. 4 'S V 3Se 1' 0 0. -105
7.96085395E+15 1. 4 'S V 1Se 3' 0 0. -105
7.85380458E+15 21. 4 'S V 3Fo 1' 0 0. -105
7.71050192E+15 5. 4 'S V 1Do 1' 0 0. -105
7.19828251E+15 9. 4 'S V 3Po 2' 0 0. -105
7.12324245E+15 15. 4 'S V 3Do 1' 0 0. -105
7.08422428E+15 9. 4 'S V 3Po 3' 0 0. -105
7.07820489E+15 3. 4 'S V 1Po 2' 0 0. -105
6.55845211E+15 7. 4 'S V 1Fo 1' 0 0. -105
6.12127222E+15 3. 5 'S V 1Po 3' 0 0. -105
5.68307281E+15 15. 5 'S V 3De 2' 0 0. -105
5.63632424E+15 5. 5 'S V 1De 3' 0 0. -105
5.14454082E+15 33. 5 'S V +3__ 2' 0 0. -105
4.95653883E+15 11. 5 'S V +1__ 1' 0 0. -105
3.64588338E+15 141. 6 'S V +3__ 4' 0 0. -105
3.56924238E+15 51. 6 'S V +1__ 3' 0 0. -105
1.92086708E+15 1039. 8 'S V +___ 5' 0 0. -105
****** Continuum transitions
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1.2079
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1.2315
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0.5220 0.6126 0.7031 0.7483 1.3118
0.4495 0.4294 0.3738 0.3614 0.3766 0.4770 0.5426 0.5752 0.5509 0.4895
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20 26 1 151 0 0 0 5.305E-19 0.000E+00
-0.0670 -0.0346 -0.0217 0.0042 0.0171 0.0300 0.0429 0.0688 0.0753 0.0882
0.1076 0.1335 0.1529 0.1787 0.1981 0.2175 0.2240 0.2305 0.2434 0.2563
0.2628 0.2757 0.2822 0.2951 0.3016 0.3081 0.3275 0.3339 0.3404 0.3533
0.3598 0.3662 0.3727 0.3792 0.4050 0.4115 0.4180 0.4244 0.4309 0.4374
0.4438 0.4503 0.4568 0.4632 0.4826 0.5214 0.5538 0.6184 0.7025 0.7348
1.3147
0.5185 0.4665 0.4368 0.4211 0.4197 0.3988 0.3311 0.1735 0.1450 0.1254
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-2.6057
21 26 1 108 0 0 0 2.233E-20 0.000E+00
-0.002 0.069 0.130 0.194 0.454 0.557 0.731 1.368
-1.116 -1.592 -1.771 -1.623 -2.077 -1.634 -1.866 -3.768
22 26 1 107 0 0 0 2.116E-19 0.000E+00
-0.002 0.062 0.183 0.500 0.578 0.756 1.418
-0.123 -1.137 -1.021 -1.380 -1.169 -1.412 -3.398
23 26 1 107 0 0 0 1.467E-20 0.000E+00
0.003 0.203 0.283 0.407 0.443 0.848 1.506
-1.317 -1.782 -1.507 -1.655 -1.254 -1.972 -3.916
24 26 1 109 0 0 0 3.380E-19 0.000E+00
-0.002 0.141 0.225 0.296 0.407 0.470 0.679 0.875 1.542
0.067 -1.127 -1.391 -0.989 -1.317 -1.011 -1.264 -1.613 -3.609
25 26 1 2 0 0 0 6.208E-19 0.000E+00
3.000 2.069 1.000 0.000
*** Line transitions
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F 1 7 0. 0.
20 23 0 0 4 0 0 0.000E+00 5.000E-02
20 24 -1 0 1 0 0 6.898E-01 2.000E-01
F 1 7 0. 0.
20 25 -1 0 1 0 0 8.872E-01 2.000E-01
F 1 7 0. 0.
21 22 0 0 4 0 0 0.000E+00 5.000E-02
21 23 -1 0 1 0 0 1.130E+00 2.000E-01
F 1 7 0. 0.
21 24 0 0 4 0 0 0.000E+00 5.000E-02
21 25 -1 0 1 0 0 8.915E-01 2.000E-01
F 1 7 0. 0.
22 23 0 0 4 0 0 0.000E+00 5.000E-02
22 24 -1 0 1 0 0 1.128E+00 2.000E-01
F 1 7 0. 0.
22 25 -1 0 1 0 0 1.057E+00 2.000E-01
F 1 7 0. 0.
23 24 0 0 4 0 0 0.000E+00 5.000E-02
23 25 -1 0 1 0 0 1.242E+00 2.000E-01
F 1 7 0. 0.
24 25 -1 0 1 0 0 1.454E+00 2.000E-01
F 1 7 0. 0.
File diff suppressed because it is too large Load Diff
+941
View File
@@ -0,0 +1,941 @@
****** Levels
8.09841317E+15 1. 3 'Si+2 1Se 1' 0 0. 0
6.51001024E+15 9. 3 'Si+2 3Po 1' 0 0. 0
5.61364413E+15 3. 3 'Si+2 1Po 1' 0 0. 0
4.43458782E+15 5. 3 'Si+2 1De 1' 0 0. -104
4.20206662E+15 9. 3 'Si+2 3Pe 1' 0 0. -104
3.81311626E+15 15. 3 'Si+2 3De 1' 0 0. -104
3.50038949E+15 3. 3 'Si+2 3Se 1' 0 0. -104
3.49834992E+15 1. 3 'Si+2 1Se 2' 0 0. -104
3.32971581E+15 1. 3 'Si+2 1Se 3' 0 0. -104
3.12900313E+15 5. 3 'Si+2 1De 2' 0 0. -104
2.84315426E+15 9. 4 'Si+2 3Po 2' 0 0. -104
2.80756536E+15 3. 4 'Si+2 1Po 2' 0 0. -104
2.13083515E+15 21. 4 'Si+2 3Fo 1' 0 0. -104
2.05475584E+15 15. 4 'Si+2 3De 2' 0 0. -104
1.97261969E+15 5. 4 'Si+2 1De 3' 0 0. -104
1.95794446E+15 7. 4 'Si+2 1Fo 1' 0 0. -104
1.95191714E+15 5. 4 'Si+2 1Do 1' 0 0. -104
1.91753284E+15 3. 4 'Si+2 3Se 2' 0 0. -104
1.86662661E+15 1. 4 'Si+2 1Se 4' 0 0. -104
1.81578654E+15 21. 4 'Si+2 3Fo 2' 0 0. -104
1.66702619E+15 3. 4 'Si+2 1Po 3' 0 0. -104
1.65324834E+15 9. 4 'Si+2 3Po 3' 0 0. -104
1.61580388E+15 9. 4 'Si+2 3Po 4' 0 0. -104
1.57948818E+15 15. 4 'Si+2 3Do 1' 0 0. -104
1.22081976E+15 84. 5 'Si+2+3__ 1' 0 0. -104
1.21239880E+15 38. 5 'Si+2+1__ 2' 0 0. -104
8.25812220E+14 123. 6 'Si+2+3__ 3' 0 0. -104
8.23981557E+14 39. 6 'Si+2+1__ 4' 0 0. -104
4.91747314E+14 519. 8 'Si+2+3__ 5' 0 0. -104
4.89277306E+14 172. 8 'Si+2+1__ 6' 0 0. -104
****** Continuum transitions
1 31 1 114 0 0 0 1.382E-19 0.000E+00
-0.0161 0.0033 0.0162 0.0226 0.0485 0.1196 0.2037 0.2684 0.3460 0.4106
0.4494 0.4817 0.5011 1.1088
-0.3320 -0.3414 -0.3749 -0.3845 -0.3664 -0.3756 -0.4419 -0.4799 -0.5667 -0.6330
-0.6791 -0.7049 -0.7459 -2.5694
2 31 1 120 0 0 0 9.255E-20 0.000E+00
-0.0201 0.0058 0.0122 0.0187 0.0252 0.0316 0.0446 0.0575 0.0640 0.0769
0.0833 0.0963 0.1092 0.1480 0.2579 0.3355 0.4454 0.5489 0.5812 1.1736
-0.5225 -0.4049 -0.3587 -0.2930 -0.2506 -0.2452 -0.3105 -0.3252 -0.3157 -0.3249
-0.3323 -0.3214 -0.2922 -0.2616 -0.3101 -0.3678 -0.4814 -0.6118 -0.6973 -2.4768
3 31 1 129 0 0 0 4.913E-20 0.000E+00
-0.0236 -0.0042 0.0087 0.0152 0.0216 0.0346 0.0410 0.0475 0.0604 0.0669
0.0798 0.0863 0.0928 0.1057 0.1122 0.1186 0.1316 0.1380 0.1704 0.1897
0.2091 0.2221 0.2350 0.2803 0.3773 0.5001 0.5906 0.6165 1.2237
-0.6554 -0.7206 -0.7534 -0.7434 -0.7014 -0.5285 -0.4678 -0.4468 -0.4694 -0.4649
-0.4324 -0.4381 -0.4645 -0.5487 -0.5651 -0.5419 -0.4359 -0.3911 -0.2964 -0.3004
-0.2795 -0.2898 -0.3105 -0.3156 -0.3803 -0.4937 -0.6072 -0.6659 -2.4885
4 31 1 139 0 0 0 6.526E-19 0.000E+00
-0.0298 -0.0168 -0.0104 0.0026 0.0090 0.0155 0.0220 0.0284 0.0349 0.0414
0.0478 0.0608 0.0672 0.0737 0.0802 0.0866 0.0996 0.1060 0.1189 0.1448
0.1513 0.1577 0.1642 0.1771 0.1836 0.2095 0.2159 0.2224 0.2289 0.2418
0.2547 0.2677 0.3000 0.3388 0.4358 0.5780 0.6750 0.7462 1.2984
-0.0530 0.0655 0.1402 0.3121 0.3753 0.4019 0.3791 0.2996 0.1625 -0.0184
-0.1350 -0.1890 -0.2091 -0.1252 -0.0777 -0.0768 -0.1281 -0.1462 -0.1147 -0.0212
-0.0136 -0.0326 -0.0802 -0.2212 -0.2548 -0.2089 -0.1879 -0.1763 -0.1785 -0.2130
-0.2157 -0.2107 -0.2259 -0.2335 -0.3088 -0.4521 -0.5901 -0.7968 -2.4561
5 31 1 140 0 0 0 7.046E-21 0.000E+00
-0.0317 -0.0252 -0.0188 -0.0123 -0.0058 0.0006 0.0071 0.0136 0.0200 0.0265
0.0330 0.0394 0.0459 0.0524 0.0588 0.0653 0.0718 0.0782 0.0847 0.0912
0.0976 0.1041 0.1106 0.1170 0.1300 0.1429 0.1494 0.1623 0.1752 0.2140
0.2463 0.2851 0.3239 0.3563 0.4015 0.4403 0.5955 0.6925 0.7313 1.3192
-2.1265 -1.8414 -1.4258 -0.9677 -0.5354 -0.1777 0.0979 0.2816 0.3721 0.3687
0.2712 0.0807 -0.1978 -0.5390 -0.7877 -0.6621 -0.3855 -0.1784 -0.0750 -0.0681
-0.1319 -0.2136 -0.2533 -0.2413 -0.1851 -0.1551 -0.1547 -0.1834 -0.2150 -0.2155
-0.2055 -0.1879 -0.1870 -0.1772 -0.1989 -0.2157 -0.3612 -0.4939 -0.6001 -2.3664
6 31 1 135 0 0 0 7.701E-19 0.000E+00
-0.0351 -0.0092 -0.0027 0.0037 0.0167 0.0231 0.0296 0.0749 0.0878 0.1007
0.1395 0.1460 0.1525 0.1589 0.1654 0.1719 0.1783 0.1848 0.1913 0.2042
0.2365 0.2430 0.2559 0.2624 0.2818 0.2882 0.3076 0.3400 0.3852 0.4305
0.5404 0.6568 0.7279 0.7667 1.3011
0.7535 0.7371 0.7183 0.6809 0.5810 0.5446 0.5198 0.4360 0.3883 0.3347
0.2319 0.2231 0.2296 0.2490 0.2776 0.2959 0.2878 0.2476 0.1826 0.1186
-0.0199 -0.0333 0.0125 0.0078 -0.0980 -0.1246 -0.1493 -0.2369 -0.2952 -0.3754
-0.5544 -0.7317 -0.8319 -0.9388 -2.5442
7 31 1 147 0 0 0 7.201E-20 0.000E+00
-0.0384 0.0133 0.0198 0.0262 0.0327 0.0456 0.0521 0.0586 0.0974 0.1038
0.1232 0.1362 0.1620 0.1685 0.1750 0.1944 0.2008 0.2073 0.2138 0.2202
0.2267 0.2332 0.2396 0.2461 0.2590 0.2655 0.2720 0.2784 0.2849 0.3043
0.3108 0.3237 0.3302 0.3366 0.3431 0.3495 0.3560 0.3625 0.3754 0.3883
0.4013 0.4271 0.5112 0.6858 0.7634 0.7957 1.3669
-0.6814 -0.4880 -0.4566 -0.4397 -0.4591 -0.5538 -0.5896 -0.6107 -0.5368 -0.5374
-0.5701 -0.5822 -0.5628 -0.5489 -0.5239 -0.4055 -0.3582 -0.2452 -0.1021 0.0803
0.2170 0.2778 0.2470 0.1214 -0.2824 -0.4971 -0.6278 -0.6747 -0.6924 -0.6166
-0.5607 -0.3415 -0.2728 -0.2742 -0.3300 -0.4023 -0.4403 -0.4265 -0.3674 -0.3428
-0.3447 -0.3900 -0.4532 -0.6376 -0.7253 -0.8133 -2.5293
8 31 1 160 0 0 0 2.199E-20 0.000E+00
-0.0388 -0.0323 -0.0259 -0.0194 -0.0129 -0.0065 0.0000 0.0065 0.0129 0.0194
0.0259 0.0323 0.0388 0.0453 0.0517 0.0582 0.0647 0.0711 0.0776 0.0841
0.0905 0.0970 0.1035 0.1099 0.1164 0.1229 0.1293 0.1358 0.1423 0.1487
0.1617 0.1681 0.1875 0.1940 0.2004 0.2069 0.2198 0.2263 0.2392 0.2457
0.2522 0.2586 0.2651 0.2716 0.2845 0.2910 0.2974 0.3233 0.3362 0.3492
0.3621 0.4138 0.4397 0.4526 0.4656 0.4785 0.5108 0.7630 0.8147 1.3617
-2.7352 -2.6698 -2.4895 -2.2146 -1.8732 -1.4661 -1.0152 -0.5837 -0.2150 0.0573
0.2272 0.2958 0.2627 0.1332 -0.0880 -0.3942 -0.7601 -1.0260 -0.8586 -0.5045
-0.2152 -0.0345 0.0433 0.0219 -0.0737 -0.1875 -0.2429 -0.2331 -0.2135 -0.2129
-0.2287 -0.2251 -0.1781 -0.1718 -0.1842 -0.2240 -0.3324 -0.3361 -0.2949 -0.2520
-0.1855 -0.1477 -0.1508 -0.1938 -0.3094 -0.3334 -0.3244 -0.2504 -0.2284 -0.2434
-0.2548 -0.1812 -0.1965 -0.1741 -0.1479 -0.1436 -0.1764 -0.5120 -0.6594 -2.3029
9 31 1 147 0 0 0 2.503E-20 0.000E+00
-0.0406 -0.0341 -0.0147 -0.0083 0.0047 0.0111 0.0176 0.0241 0.0305 0.0370
0.0435 0.0499 0.0564 0.0693 0.0952 0.1016 0.1081 0.1210 0.1404 0.1728
0.1922 0.2116 0.2180 0.2568 0.2633 0.2698 0.2762 0.2827 0.2892 0.2956
0.3021 0.3150 0.3215 0.3280 0.3344 0.3409 0.3474 0.3538 0.3668 0.3732
0.3797 0.4443 0.5025 0.6448 0.7806 0.8129 1.4034
-1.7696 -1.6711 -1.3370 -1.2221 -0.9429 -0.7830 -0.6324 -0.5252 -0.4905 -0.5347
-0.6503 -0.8022 -0.9374 -0.9938 -0.7944 -0.7734 -0.7824 -0.8380 -0.8578 -0.8668
-0.8821 -0.8526 -0.8350 -0.5763 -0.4347 -0.3146 -0.2557 -0.2566 -0.3141 -0.4151
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-0.4571 -0.4774 -0.4877 -0.5837 -0.7277 -0.8138 -2.5879
10 31 1 145 0 0 0 5.436E-19 0.000E+00
-0.0436 -0.0178 -0.0113 0.0081 0.0146 0.0210 0.0275 0.0340 0.0404 0.0469
0.0534 0.0857 0.0986 0.1051 0.1180 0.1245 0.1439 0.1762 0.1956 0.2085
0.2150 0.2279 0.2473 0.2732 0.2861 0.2991 0.3055 0.3120 0.3249 0.3379
0.3637 0.3831 0.3896 0.4025 0.4090 0.4155 0.4413 0.4478 0.4672 0.4801
0.4995 0.7646 0.8034 0.8487 1.4109
0.9549 0.8152 0.7563 0.5229 0.4993 0.5506 0.6400 0.7137 0.7466 0.7380
0.7019 0.4786 0.3921 0.3754 0.3741 0.3574 0.2642 0.1700 0.1423 0.1258
0.1070 0.0377 -0.0779 -0.1555 -0.1582 -0.1358 -0.1326 -0.1462 -0.1960 -0.2051
-0.2151 -0.2069 -0.2197 -0.2658 -0.2816 -0.2881 -0.2516 -0.2577 -0.3081 -0.3140
-0.3155 -0.6231 -0.6793 -0.8060 -2.4953
11 31 1 145 0 0 0 1.669E-19 0.000E+00
-0.0478 -0.0284 0.0169 0.0621 0.0880 0.1268 0.1397 0.1591 0.1656 0.1850
0.1915 0.2109 0.2691 0.2820 0.3014 0.3079 0.3208 0.3272 0.3337 0.3402
0.3466 0.3531 0.3596 0.3660 0.3725 0.3790 0.3854 0.3919 0.3984 0.4048
0.4113 0.4178 0.4242 0.4307 0.4372 0.4436 0.4501 0.4566 0.4695 0.5471
0.6699 0.7605 0.8381 0.8704 1.4514
-0.0332 -0.0984 -0.3072 -0.4296 -0.4913 -0.5402 -0.5443 -0.5180 -0.5217 -0.5960
-0.6146 -0.6320 -0.6080 -0.5941 -0.4863 -0.4417 -0.2070 -0.0728 0.0077 0.0108
-0.0625 -0.1988 -0.3684 -0.5277 -0.6357 -0.6926 -0.7036 -0.7012 -0.6443 -0.5434
-0.4010 -0.2726 -0.1947 -0.1858 -0.2383 -0.3150 -0.3806 -0.3953 -0.3740 -0.4110
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12 31 1 165 0 0 0 2.885E-19 0.000E+00
-0.0485 -0.0421 -0.0356 -0.0227 0.0032 0.0161 0.0355 0.0420 0.0484 0.0549
0.0743 0.0808 0.0872 0.0937 0.1002 0.1066 0.1131 0.1390 0.1519 0.1648
0.1778 0.1842 0.1972 0.2036 0.2101 0.2166 0.2230 0.2295 0.2360 0.2424
0.2489 0.2554 0.2683 0.2748 0.2812 0.2942 0.3006 0.3071 0.3136 0.3200
0.3265 0.3330 0.3394 0.3524 0.3588 0.3718 0.3782 0.3911 0.3976 0.4041
0.4105 0.4235 0.4299 0.4364 0.4493 0.4558 0.4687 0.4752 0.4946 0.5657
0.7145 0.7726 0.8438 0.8761 1.4569
0.5440 0.5061 0.4564 0.3321 0.0441 -0.0825 -0.2042 -0.2357 -0.2535 -0.2556
-0.1539 -0.1569 -0.2008 -0.2675 -0.3152 -0.3458 -0.3620 -0.3955 -0.4416 -0.4588
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0.1498 0.1920 0.1501 -0.0759 -0.1626 -0.2283 -0.2841 -0.4621 -0.5328 -0.5467
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13 31 1 164 0 0 0 1.596E-18 0.000E+00
-0.0642 -0.0254 -0.0060 0.0005 0.0070 0.0134 0.0199 0.0328 0.0393 0.0458
0.0522 0.0587 0.0652 0.0716 0.0781 0.0846 0.0910 0.1040 0.1104 0.1169
0.1234 0.1298 0.1363 0.1428 0.1492 0.1557 0.1622 0.1686 0.1751 0.1816
0.1880 0.1945 0.2010 0.2074 0.2139 0.2204 0.2268 0.2333 0.2398 0.2462
0.2527 0.2721 0.3238 0.3497 0.3626 0.3691 0.4143 0.4208 0.4273 0.4467
0.4531 0.4725 0.4790 0.4855 0.5049 0.5178 0.5372 0.5631 0.5760 0.5889
0.9122 0.9445 1.0415 1.5210
0.6409 0.6546 0.7051 0.7361 0.7854 0.8486 0.9396 1.1606 1.2386 1.2614
1.2202 1.1117 0.9368 0.7187 0.5100 0.3701 0.2931 0.1670 0.1611 0.1748
0.3083 0.4749 0.6762 0.8523 0.9612 0.9909 0.9393 0.8186 0.6704 0.6051
0.7038 0.8645 0.9784 1.0085 0.9577 0.8485 0.7208 0.6132 0.5424 0.5020
0.4818 0.4580 0.3465 0.3336 0.3496 0.3450 0.1314 0.1310 0.1144 0.0354
0.0300 0.0625 0.0618 0.0423 -0.0673 -0.1161 -0.1503 -0.1542 -0.1772 -0.2100
-0.6339 -0.6916 -0.9766 -2.4175
14 31 1 160 0 0 0 5.505E-21 0.000E+00
-0.0677 -0.0354 -0.0289 -0.0224 -0.0160 -0.0095 -0.0030 0.0034 0.0099 0.0164
0.0228 0.0293 0.0357 0.0422 0.0551 0.0681 0.0745 0.1069 0.1392 0.1457
0.1651 0.1780 0.2039 0.2233 0.2621 0.2685 0.2879 0.2944 0.3203 0.3461
0.3720 0.3914 0.4108 0.4366 0.4496 0.4560 0.4625 0.4690 0.4754 0.4819
0.4884 0.4948 0.5013 0.5078 0.5207 0.5272 0.5336 0.5595 0.5660 0.5724
0.5789 0.5854 0.5918 0.5983 0.6048 0.6177 0.8569 0.9604 0.9927 1.5315
0.7273 0.5893 0.6025 0.7050 0.8529 1.1551 1.4330 1.6382 1.7699 1.8365
1.8449 1.7968 1.6871 1.5100 1.1200 0.8792 0.7697 0.6470 0.5773 0.5541
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0.7405 0.2730 0.2388 0.3172 0.5515 0.8358 1.0960 1.3026 1.4500 1.5409
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0.6481 0.6130 0.5988 0.5816 0.4731 0.3992 0.3575 0.3202 0.2794 0.1301
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16 31 1 173 0 0 0 4.809E-20 0.000E+00
-0.0710 -0.0193 -0.0128 0.0001 0.0066 0.0130 0.0195 0.0259 0.0324 0.0389
0.0453 0.0518 0.0583 0.0647 0.0712 0.0777 0.0841 0.0906 0.0971 0.1035
0.1229 0.1423 0.1553 0.1617 0.1811 0.1876 0.1941 0.2005 0.2070 0.2264
0.2329 0.2458 0.2652 0.2781 0.2911 0.3493 0.3751 0.3816 0.3945 0.4010
0.4204 0.4268 0.4333 0.4462 0.4527 0.4592 0.4721 0.4786 0.4850 0.4980
0.5044 0.5109 0.5174 0.5238 0.5368 0.5432 0.5497 0.5562 0.5626 0.5756
0.5885 0.5950 0.6014 0.6079 0.6144 0.6208 0.6273 0.6402 0.6984 0.8795
0.9700 0.9959 1.6095
0.5610 0.1750 0.1504 0.1679 0.3704 0.7388 1.0660 1.3100 1.4680 1.5470
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1.6355
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-2.497 -4.292
*** Line transitions
1 2 0 0 4 0 0 0.000E+00 5.000E-02
1 3 -1 1 1 0 0 1.700E+00 7.000E-01
T 3 15 175. 0.
2.6E+9 1.1E-6 0. 0. 0.
1 4 0 0 4 0 0 0.000E+00 5.000E-02
1 5 0 0 4 0 0 0.000E+00 5.000E-02
1 6 0 0 4 0 0 0.000E+00 5.000E-02
1 7 0 0 4 0 0 0.000E+00 5.000E-02
1 8 0 0 4 0 0 0.000E+00 5.000E-02
1 9 0 0 4 0 0 0.000E+00 5.000E-02
1 10 0 0 4 0 0 0.000E+00 5.000E-02
1 11 0 0 4 0 0 0.000E+00 5.000E-02
1 12 -1 1 1 0 0 1.560E-02 2.000E-01
T 3 11 40. 0.
6.6E+8 0. 0. 0. 0.
1 13 0 0 4 0 0 0.000E+00 5.000E-02
1 14 0 0 4 0 0 0.000E+00 5.000E-02
1 15 0 0 4 0 0 0.000E+00 5.000E-02
1 16 0 0 4 0 0 0.000E+00 5.000E-02
1 17 0 0 4 0 0 0.000E+00 5.000E-02
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1 20 0 0 4 0 0 0.000E+00 5.000E-02
1 21 -1 0 1 0 0 1.410E-02 2.000E-01
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1 26 -1 0 1 0 0 7.078E-03 2.000E-01
F 1 7 0. 0.
1 27 0 0 4 0 0 0.000E+00 5.000E-02
1 28 -1 0 1 0 0 2.870E-03 2.000E-01
F 1 7 0. 0.
1 29 0 0 4 0 0 0.000E+00 5.000E-02
1 30 -1 0 1 0 0 4.920E-03 2.000E-01
F 1 7 0. 0.
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F 1 7 0. 0.
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22 27 -1 0 1 0 0 6.567E-02 2.000E-01
F 1 7 0. 0.
22 28 0 0 4 0 0 0.000E+00 5.000E-02
22 29 -1 0 1 0 0 8.098E-02 2.000E-01
F 1 7 0. 0.
22 30 0 0 4 0 0 0.000E+00 5.000E-02
23 24 0 0 4 0 0 0.000E+00 5.000E-02
23 25 -1 0 1 0 0 4.033E-01 2.000E-01
F 1 7 0. 0.
23 26 0 0 4 0 0 0.000E+00 5.000E-02
23 27 -1 0 1 0 0 1.670E-02 2.000E-01
F 1 7 0. 0.
23 28 0 0 4 0 0 0.000E+00 5.000E-02
23 29 -1 0 1 0 0 1.392E-01 2.000E-01
F 1 7 0. 0.
23 30 0 0 4 0 0 0.000E+00 5.000E-02
24 25 -1 0 1 0 0 1.453E-04 2.000E-01
F 1 7 0. 0.
24 26 0 0 4 0 0 0.000E+00 5.000E-02
24 27 -1 0 1 0 0 3.016E-02 2.000E-01
F 1 7 0. 0.
24 28 0 0 4 0 0 0.000E+00 5.000E-02
24 29 -1 0 1 0 0 1.198E-01 2.000E-01
F 1 7 0. 0.
24 30 0 0 4 0 0 0.000E+00 5.000E-02
25 26 0 0 4 0 0 0.000E+00 5.000E-02
25 27 -1 0 1 0 0 1.200E+00 2.000E-01
F 1 7 0. 0.
25 28 0 0 4 0 0 0.000E+00 5.000E-02
25 29 -1 0 1 0 0 3.393E-01 2.000E-01
F 1 7 0. 0.
25 30 0 0 4 0 0 0.000E+00 5.000E-02
26 27 0 0 4 0 0 0.000E+00 5.000E-02
26 28 -1 0 1 0 0 9.091E-01 2.000E-01
F 1 7 0. 0.
26 29 0 0 4 0 0 0.000E+00 5.000E-02
26 30 -1 0 1 0 0 2.715E-01 2.000E-01
F 1 7 0. 0.
27 28 0 0 4 0 0 0.000E+00 5.000E-02
27 29 -1 0 1 0 0 2.267E+00 2.000E-01
F 1 7 0. 0.
27 30 0 0 4 0 0 0.000E+00 5.000E-02
28 29 0 0 4 0 0 0.000E+00 5.000E-02
28 30 -1 0 1 0 0 2.469E+00 2.000E-01
F 1 7 0. 0.
29 30 0 0 4 0 0 0.000E+00 5.000E-02
+488
View File
@@ -0,0 +1,488 @@
****** Levels
1.09152381E+16 2. 3 'SiIV 2Se 1' 0 0. 0
8.77809108E+15 2. 3 'SiIV 2Po 1' 0 0. 0
8.76426765E+15 4. 3 'SiIV 2Po 1' 0 0. 0
6.10731927E+15 10. 3 'SiIV 2De 1' 0 0. 0
5.09989643E+15 2. 4 'SiIV 2Se 2' 0 0. -105
4.36852734E+15 6. 4 'SiIV 2Po 2' 0 0. -105
3.42018370E+15 10. 4 'SiIV 2De 2' 0 0. -105
3.29666540E+15 14. 4 'SiIV 2Fo 1' 0 0. -105
2.95820699E+15 2. 5 'SiIV 2Se 3' 0 0. -105
2.62435926E+15 6. 5 'SiIV 2Po 3' 0 0. -105
2.17635984E+15 10. 5 'SiIV 2De 3' 0 0. -105
2.10976304E+15 14. 5 'SiIV 2Fo 2' 0 0. -105
2.10619761E+15 18. 5 'SiIV 2Ge 1' 0 0. -105
1.93114786E+15 2. 6 'SiIV 2Se 4' 0 0. -105
1.75152429E+15 6. 6 'SiIV 2Po 4' 0 0. -105
1.50430420E+15 10. 6 'SiIV 2De 4' 0 0. -105
1.46487100E+15 14. 6 'SiIV 2Fo 3' 0 0. -105
1.46262225E+15 18. 6 'SiIV 2Ge 2' 0 0. -105
1.46226010E+15 22. 6 'SiIV 2Ho 1' 0 0. -105
1.10012138E+15 98. 7 'SiIV+2__ 1' 0 0. -105
8.34428394E+14 128. 8 'SiIV+2__ 2' 0 0. -105
6.55851371E+14 162. 9 'SiIV+2__ 3' 0 0. -105
5.29803610E+14 200. 10 'SiIV+2__ 4' 0 0. -105
****** Continuum transitions
1 24 1 104 0 0 0 8.855E-20 0.000E+00
-0.0216 0.0301 0.1724 2.7420
-0.5061 -0.5400 -0.6794 -3.5594
2 24 1 105 0 0 0 1.514E-19 0.000E+00
-0.0271 0.0505 0.1475 0.2380 2.5872
-0.2749 -0.3062 -0.3788 -0.4792 -3.3148
3 24 1 105 0 0 0 1.514E-19 0.000E+00
-0.0271 0.0505 0.1475 0.2380 2.5872
-0.2749 -0.3062 -0.3788 -0.4792 -3.3148
4 24 1 106 0 0 0 4.518E-19 0.000E+00
-0.0390 -0.0196 0.0256 0.1873 0.5623 0.9195
0.2732 0.2392 0.1043 -0.4258 -1.7074 -2.9348
5 24 1 105 0 0 0 1.179E-19 0.000E+00
-0.0475 -0.0023 0.1335 0.3340 2.1809
-0.3647 -0.3985 -0.5532 -0.8242 -3.4626
6 24 1 105 0 0 0 1.689E-19 0.000E+00
-0.0561 0.0021 0.1832 0.3190 2.4293
-0.1966 -0.2381 -0.4058 -0.5619 -3.2642
7 24 1 106 0 0 0 8.163E-19 0.000E+00
-0.0725 -0.0466 0.0698 0.2249 0.4125 1.0304
0.5979 0.5572 0.2656 -0.1574 -0.7082 -2.5683
8 24 1 109 0 0 0 9.533E-21 0.000E+00
-0.0756 -0.0562 -0.0109 0.1313 0.2671 0.3835 0.4870 0.7909 0.8579
-1.2914 -1.3247 -1.4534 -1.8972 -2.3515 -2.7731 -3.1687 -4.3476 -4.6080
9 24 1 106 0 0 0 1.454E-19 0.000E+00
-0.0854 -0.0401 0.1021 0.2961 1.9708 2.0239
-0.2234 -0.2594 -0.4280 -0.6981 -3.2779 -3.3603
10 24 1 106 0 0 0 2.045E-19 0.000E+00
-0.0976 -0.0588 0.0964 0.3938 0.5813 2.2094
-0.0280 -0.0713 -0.2769 -0.6456 -0.9115 -3.2666
11 24 1 107 0 0 0 1.133E-18 0.000E+00
-0.1203 -0.0880 0.0801 0.2547 0.4228 0.6104 1.0980
0.8345 0.7854 0.4060 -0.0235 -0.4704 -1.0014 -2.4139
12 24 1 108 0 0 0 2.946E-20 0.000E+00
-0.1247 -0.0924 0.0757 0.2503 0.3990 0.5219 0.8711 0.9182
-0.6709 -0.7344 -1.2226 -1.7679 -2.2628 -2.7029 -4.0002 -4.1759
13 24 1 2 0 0 0 7.411E-19 0.000E+00
3.000 2.470 1.000 0.000
14 24 1 109 0 0 0 1.735E-19 0.000E+00
-0.1249 -0.1055 -0.0797 -0.0732 -0.0473 0.1143 0.3406 1.2006 1.9712
0.7844 0.4327 -0.0689 -0.1145 -0.1634 -0.3713 -0.7055 -2.0826 -3.3245
15 24 1 109 0 0 0 2.629E-19 0.000E+00
-0.1249 -0.1185 -0.0926 -0.0861 -0.0409 0.1143 0.3342 0.6251 2.0741
0.6586 0.5532 0.1987 0.1158 0.0200 -0.2333 -0.5462 -0.9544 -3.0646
16 24 1 110 0 0 0 1.447E-18 0.000E+00
-0.1249 -0.1055 -0.0861 -0.0667 -0.0603 0.1402 0.3341 0.5152 0.7286 1.2096
1.7630 1.4388 1.1464 0.8600 0.8305 0.3893 -0.0701 -0.5321 -1.1160 -2.4716
17 24 1 111 0 0 0 5.942E-20 0.000E+00
-0.1249 -0.1055 -0.0732 -0.0667 0.1208 0.3083 0.4764 0.6187 0.7286 0.8062
0.9693
0.4109 0.0813 -0.4028 -0.4914 -1.0288 -1.6026 -2.1475 -2.6386 -3.0370 -3.3319
-3.9393
18 24 1 2 0 0 0 8.893E-19 0.000E+00
3.000 2.964 1.000 0.000
19 24 1 2 0 0 0 8.894E-19 0.000E+00
3.000 2.965 1.000 0.000
20 24 1 105 0 0 0 5.438E-20 0.000E+00
0.003 0.301 0.706 1.297 2.000
-0.748 -1.488 -2.412 -3.592 -4.771
21 24 1 105 0 0 0 5.717E-20 0.000E+00
-0.006 0.354 0.803 1.355 1.982
-0.704 -1.611 -2.658 -3.776 -4.824
22 24 1 104 0 0 0 5.725E-20 0.000E+00
-0.009 0.413 1.069 2.041
-0.697 -1.743 -3.275 -5.060
23 24 1 105 0 0 0 6.346E-20 0.000E+00
-0.004 0.199 0.744 1.400 2.046
-0.666 -1.183 -2.546 -3.982 -5.134
*** Line transitions
1 2 -1 1 1 0 0 2.600E-01 7.000E-01
T 3 19 400. 0.
9.1E+8 1.0E-6 0. 0. 0.
1 3 -1 1 1 0 0 5.200E-01 7.000E-01
T 3 19 400. 0.
9.1E+8 1.0E-6 0. 0. 0.
1 4 0 0 4 0 0 0.000E+00 5.000E-02
1 5 0 0 4 0 0 0.000E+00 5.000E-02
1 6 -1 0 1 0 0 3.510E-02 2.000E-01
F 1 7 0. 0.
1 7 0 0 4 0 0 0.000E+00 5.000E-02
1 8 0 0 4 0 0 0.000E+00 5.000E-02
1 9 0 0 4 0 0 0.000E+00 5.000E-02
1 10 -1 0 1 0 0 1.600E-02 2.000E-01
F 1 7 0. 0.
1 11 0 0 4 0 0 0.000E+00 5.000E-02
1 12 0 0 4 0 0 0.000E+00 5.000E-02
1 13 0 0 4 0 0 0.000E+00 5.000E-02
1 14 0 0 4 0 0 0.000E+00 5.000E-02
1 15 -1 0 1 0 0 8.300E-03 2.000E-01
F 1 7 0. 0.
1 16 0 0 4 0 0 0.000E+00 5.000E-02
1 17 0 0 4 0 0 0.000E+00 5.000E-02
1 18 0 0 4 0 0 0.000E+00 5.000E-02
1 19 0 0 4 0 0 0.000E+00 5.000E-02
1 20 -1 0 1 0 0 4.850E-03 2.000E-01
F 1 7 0. 0.
1 21 -1 0 1 0 0 3.085E-03 2.000E-01
F 1 7 0. 0.
1 22 -1 0 1 0 0 2.085E-03 2.000E-01
F 1 7 0. 0.
1 23 -1 0 1 0 0 1.480E-03 2.000E-01
F 1 7 0. 0.
2 3 0 0 4 0 0 0.000E+00 5.000E-02
2 4 -1 0 1 0 0 7.933E-01 7.000E-01
F 1 7 0. 0.
2 5 -1 0 1 0 0 1.195E-01 2.000E-01
F 1 7 0. 0.
2 6 0 0 4 0 0 0.000E+00 5.000E-02
2 7 -1 0 1 0 0 8.483E-03 2.000E-01
F 1 7 0. 0.
2 8 0 0 4 0 0 0.000E+00 5.000E-02
2 9 -1 0 1 0 0 1.833E-02 2.000E-01
F 1 7 0. 0.
2 10 0 0 4 0 0 0.000E+00 5.000E-02
2 11 -1 0 1 0 0 9.650E-03 2.000E-01
F 1 7 0. 0.
2 12 0 0 4 0 0 0.000E+00 5.000E-02
2 13 0 0 4 0 0 0.000E+00 5.000E-02
2 14 -1 0 1 0 0 6.733E-03 2.000E-01
F 1 7 0. 0.
2 15 0 0 4 0 0 0.000E+00 5.000E-02
2 16 -1 0 1 0 0 6.467E-03 2.000E-01
F 1 7 0. 0.
2 17 0 0 4 0 0 0.000E+00 5.000E-02
2 18 0 0 4 0 0 0.000E+00 5.000E-02
2 19 0 0 4 0 0 0.000E+00 5.000E-02
2 20 -1 0 1 0 0 7.617E-03 2.000E-01
F 1 7 0. 0.
2 21 -1 0 1 0 0 4.850E-03 2.000E-01
F 1 7 0. 0.
2 22 -1 0 1 0 0 3.305E-03 2.000E-01
F 1 7 0. 0.
2 23 -1 0 1 0 0 2.352E-03 2.000E-01
F 1 7 0. 0.
3 4 -1 0 1 0 0 7.933E-01 7.000E-01
F 1 7 0. 0.
3 5 -1 0 1 0 0 1.195E-01 2.000E-01
F 1 7 0. 0.
3 6 0 0 4 0 0 0.000E+00 5.000E-02
3 7 -1 0 1 0 0 8.483E-03 2.000E-01
F 1 7 0. 0.
3 8 0 0 4 0 0 0.000E+00 5.000E-02
3 9 -1 0 1 0 0 1.833E-02 2.000E-01
F 1 7 0. 0.
3 10 0 0 4 0 0 0.000E+00 5.000E-02
3 11 -1 0 1 0 0 9.650E-03 2.000E-01
F 1 7 0. 0.
3 12 0 0 4 0 0 0.000E+00 5.000E-02
3 13 0 0 4 0 0 0.000E+00 5.000E-02
3 14 -1 0 1 0 0 6.733E-03 2.000E-01
F 1 7 0. 0.
3 15 0 0 4 0 0 0.000E+00 5.000E-02
3 16 -1 0 1 0 0 6.467E-03 2.000E-01
F 1 7 0. 0.
3 17 0 0 4 0 0 0.000E+00 5.000E-02
3 18 0 0 4 0 0 0.000E+00 5.000E-02
3 19 0 0 4 0 0 0.000E+00 5.000E-02
3 20 -1 0 1 0 0 7.617E-03 2.000E-01
F 1 7 0. 0.
3 21 -1 0 1 0 0 4.850E-03 2.000E-01
F 1 7 0. 0.
3 22 -1 0 1 0 0 3.305E-03 2.000E-01
F 1 7 0. 0.
3 23 -1 0 1 0 0 2.352E-03 2.000E-01
F 1 7 0. 0.
4 5 0 0 4 0 0 0.000E+00 5.000E-02
4 6 -1 0 1 0 0 1.410E-01 2.000E-01
F 1 7 0. 0.
4 7 0 0 4 0 0 0.000E+00 5.000E-02
4 8 -1 0 1 0 0 9.020E-01 2.000E-01
F 1 7 0. 0.
4 9 0 0 4 0 0 0.000E+00 5.000E-02
4 10 -1 0 1 0 0 1.260E-02 2.000E-01
F 1 7 0. 0.
4 11 0 0 4 0 0 0.000E+00 5.000E-02
4 12 -1 0 1 0 0 1.680E-01 2.000E-01
F 1 7 0. 0.
4 13 0 0 4 0 0 0.000E+00 5.000E-02
4 14 0 0 4 0 0 0.000E+00 5.000E-02
4 15 -1 0 1 0 0 4.030E-03 2.000E-01
F 1 7 0. 0.
4 16 0 0 4 0 0 0.000E+00 5.000E-02
4 17 -1 0 1 0 0 6.220E-02 2.000E-01
F 1 7 0. 0.
4 18 0 0 4 0 0 0.000E+00 5.000E-02
4 19 0 0 4 0 0 0.000E+00 5.000E-02
4 20 -1 0 1 0 0 3.258E-02 2.000E-01
F 1 7 0. 0.
4 21 -1 0 1 0 0 1.875E-02 2.000E-01
F 1 7 0. 0.
4 22 -1 0 1 0 0 1.186E-02 2.000E-01
F 1 7 0. 0.
4 23 -1 0 1 0 0 8.070E-03 2.000E-01
F 1 7 0. 0.
5 6 -1 0 1 0 0 1.180E+00 7.000E-01
F 1 7 0. 0.
5 7 0 0 4 0 0 0.000E+00 5.000E-02
5 8 0 0 4 0 0 0.000E+00 5.000E-02
5 9 0 0 4 0 0 0.000E+00 5.000E-02
5 10 -1 0 1 0 0 2.335E-02 2.000E-01
F 1 7 0. 0.
5 11 0 0 4 0 0 0.000E+00 5.000E-02
5 12 0 0 4 0 0 0.000E+00 5.000E-02
5 13 0 0 4 0 0 0.000E+00 5.000E-02
5 14 0 0 4 0 0 0.000E+00 5.000E-02
5 15 -1 0 1 0 0 1.305E-02 2.000E-01
F 1 7 0. 0.
5 16 0 0 4 0 0 0.000E+00 5.000E-02
5 17 0 0 4 0 0 0.000E+00 5.000E-02
5 18 0 0 4 0 0 0.000E+00 5.000E-02
5 19 0 0 4 0 0 0.000E+00 5.000E-02
5 20 -1 0 1 0 0 7.350E-03 2.000E-01
F 1 7 0. 0.
5 21 -1 0 1 0 0 4.505E-03 2.000E-01
F 1 7 0. 0.
5 22 -1 0 1 0 0 2.970E-03 2.000E-01
F 1 7 0. 0.
5 23 -1 0 1 0 0 2.070E-03 2.000E-01
F 1 7 0. 0.
6 7 -1 0 1 0 0 1.183E+00 7.000E-01
F 1 7 0. 0.
6 8 0 0 4 0 0 0.000E+00 5.000E-02
6 9 -1 0 1 0 0 2.100E-01 2.000E-01
F 1 7 0. 0.
6 10 0 0 4 0 0 0.000E+00 5.000E-02
6 11 -1 0 1 0 0 4.300E-06 2.000E-01
F 1 7 0. 0.
6 12 0 0 4 0 0 0.000E+00 5.000E-02
6 13 0 0 4 0 0 0.000E+00 5.000E-02
6 14 -1 0 1 0 0 3.117E-02 2.000E-01
F 1 7 0. 0.
6 15 0 0 4 0 0 0.000E+00 5.000E-02
6 16 -1 0 1 0 0 2.133E-03 2.000E-01
F 1 7 0. 0.
6 17 0 0 4 0 0 0.000E+00 5.000E-02
6 18 0 0 4 0 0 0.000E+00 5.000E-02
6 19 0 0 4 0 0 0.000E+00 5.000E-02
6 20 -1 0 1 0 0 1.358E-02 2.000E-01
F 1 7 0. 0.
6 21 -1 0 1 0 0 7.417E-03 2.000E-01
F 1 7 0. 0.
6 22 -1 0 1 0 0 4.628E-03 2.000E-01
F 1 7 0. 0.
6 23 -1 0 1 0 0 3.142E-03 2.000E-01
F 1 7 0. 0.
7 8 -1 0 1 0 0 1.300E-01 7.000E-01
F 1 7 0. 0.
7 9 0 0 4 0 0 0.000E+00 5.000E-02
7 10 -1 0 1 0 0 2.920E-01 2.000E-01
F 1 7 0. 0.
7 11 0 0 4 0 0 0.000E+00 5.000E-02
7 12 -1 0 1 0 0 6.950E-01 2.000E-01
F 1 7 0. 0.
7 13 0 0 4 0 0 0.000E+00 5.000E-02
7 14 0 0 4 0 0 0.000E+00 5.000E-02
7 15 -1 0 1 0 0 2.650E-02 2.000E-01
F 1 7 0. 0.
7 16 0 0 4 0 0 0.000E+00 5.000E-02
7 17 -1 0 1 0 0 1.770E-01 2.000E-01
F 1 7 0. 0.
7 18 0 0 4 0 0 0.000E+00 5.000E-02
7 19 0 0 4 0 0 0.000E+00 5.000E-02
7 20 -1 0 1 0 0 8.269E-02 2.000E-01
F 1 7 0. 0.
7 21 -1 0 1 0 0 4.315E-02 2.000E-01
F 1 7 0. 0.
7 22 -1 0 1 0 0 2.579E-02 2.000E-01
F 1 7 0. 0.
7 23 -1 0 1 0 0 1.695E-02 2.000E-01
F 1 7 0. 0.
8 9 0 0 4 0 0 0.000E+00 5.000E-02
8 10 0 0 4 0 0 0.000E+00 5.000E-02
8 11 -1 0 1 0 0 2.143E-02 2.000E-01
F 1 7 0. 0.
8 12 0 0 4 0 0 0.000E+00 5.000E-02
8 13 -1 0 1 0 0 1.344E+00 2.000E-01
F 1 7 0. 0.
8 14 0 0 4 0 0 0.000E+00 5.000E-02
8 15 0 0 4 0 0 0.000E+00 5.000E-02
8 16 -1 0 1 0 0 3.600E-03 2.000E-01
F 1 7 0. 0.
8 17 0 0 4 0 0 0.000E+00 5.000E-02
8 18 -1 0 1 0 0 2.117E-01 2.000E-01
F 1 7 0. 0.
8 19 0 0 4 0 0 0.000E+00 5.000E-02
8 20 -1 0 1 0 0 7.612E-02 2.000E-01
F 1 7 0. 0.
8 21 -1 0 1 0 0 3.692E-02 2.000E-01
F 1 7 0. 0.
8 22 -1 0 1 0 0 2.117E-02 2.000E-01
F 1 7 0. 0.
8 23 -1 0 1 0 0 1.345E-02 2.000E-01
F 1 7 0. 0.
9 10 -1 0 1 0 0 1.540E+00 7.000E-01
F 1 7 0. 0.
9 11 0 0 4 0 0 0.000E+00 5.000E-02
9 12 0 0 4 0 0 0.000E+00 5.000E-02
9 13 0 0 4 0 0 0.000E+00 5.000E-02
9 14 0 0 4 0 0 0.000E+00 5.000E-02
9 15 -1 0 1 0 0 1.800E-02 2.000E-01
F 1 7 0. 0.
9 16 0 0 4 0 0 0.000E+00 5.000E-02
9 17 0 0 4 0 0 0.000E+00 5.000E-02
9 18 0 0 4 0 0 0.000E+00 5.000E-02
9 19 0 0 4 0 0 0.000E+00 5.000E-02
9 20 -1 0 1 0 0 1.145E-02 2.000E-01
F 1 7 0. 0.
9 21 -1 0 1 0 0 6.750E-03 2.000E-01
F 1 7 0. 0.
9 22 -1 0 1 0 0 4.290E-03 2.000E-01
F 1 7 0. 0.
9 23 -1 0 1 0 0 2.900E-03 2.000E-01
F 1 7 0. 0.
10 11 -1 0 1 0 0 1.520E+00 7.000E-01
F 1 7 0. 0.
10 12 0 0 4 0 0 0.000E+00 5.000E-02
10 13 0 0 4 0 0 0.000E+00 5.000E-02
10 14 -1 0 1 0 0 2.983E-01 2.000E-01
F 1 7 0. 0.
10 15 0 0 4 0 0 0.000E+00 5.000E-02
10 16 -1 0 1 0 0 3.650E-03 2.000E-01
F 1 7 0. 0.
10 17 0 0 4 0 0 0.000E+00 5.000E-02
10 18 0 0 4 0 0 0.000E+00 5.000E-02
10 19 0 0 4 0 0 0.000E+00 5.000E-02
10 20 -1 0 1 0 0 4.397E-02 2.000E-01
F 1 7 0. 0.
10 21 -1 0 1 0 0 1.649E-02 2.000E-01
F 1 7 0. 0.
10 22 -1 0 1 0 0 8.567E-03 2.000E-01
F 1 7 0. 0.
10 23 -1 0 1 0 0 5.200E-03 2.000E-01
F 1 7 0. 0.
11 12 -1 0 1 0 0 2.360E-01 7.000E-01
F 1 7 0. 0.
11 13 0 0 4 0 0 0.000E+00 5.000E-02
11 14 0 0 4 0 0 0.000E+00 5.000E-02
11 15 -1 0 1 0 0 4.430E-01 2.000E-01
F 1 7 0. 0.
11 16 0 0 4 0 0 0.000E+00 5.000E-02
11 17 -1 0 1 0 0 6.050E-01 2.000E-01
F 1 7 0. 0.
11 18 0 0 4 0 0 0.000E+00 5.000E-02
11 19 0 0 4 0 0 0.000E+00 5.000E-02
11 20 -1 0 1 0 0 2.114E-01 2.000E-01
F 1 7 0. 0.
11 21 -1 0 1 0 0 8.900E-02 2.000E-01
F 1 7 0. 0.
11 22 -1 0 1 0 0 4.773E-02 2.000E-01
F 1 7 0. 0.
11 23 -1 0 1 0 0 2.925E-02 2.000E-01
F 1 7 0. 0.
12 13 0 0 1 0 0 0.000E+00 7.000E-01
12 14 0 0 4 0 0 0.000E+00 5.000E-02
12 15 0 0 4 0 0 0.000E+00 5.000E-02
12 16 -1 0 1 0 0 5.243E-02 2.000E-01
F 1 7 0. 0.
12 17 0 0 4 0 0 0.000E+00 5.000E-02
12 18 -1 0 1 0 0 1.591E+00 2.000E-01
F 1 7 0. 0.
12 19 0 0 4 0 0 0.000E+00 5.000E-02
12 20 -1 0 1 0 0 2.523E-01 2.000E-01
F 1 7 0. 0.
12 21 -1 0 1 0 0 8.793E-02 2.000E-01
F 1 7 0. 0.
12 22 -1 0 1 0 0 4.232E-02 2.000E-01
F 1 7 0. 0.
12 23 -1 0 1 0 0 2.417E-02 2.000E-01
F 1 7 0. 0.
13 14 0 0 4 0 0 0.000E+00 5.000E-02
13 15 0 0 4 0 0 0.000E+00 5.000E-02
13 16 0 0 4 0 0 0.000E+00 5.000E-02
13 17 -1 0 1 0 0 1.591E+00 2.000E-01
F 1 7 0. 0.
13 18 0 0 4 0 0 0.000E+00 5.000E-02
13 19 -1 0 1 0 0 1.591E+00 2.000E-01
F 1 7 0. 0.
13 20 -1 0 1 0 0 4.864E-01 2.000E-01
F 1 7 0. 0.
13 21 -1 0 1 0 0 1.692E-01 2.000E-01
F 1 7 0. 0.
13 22 -1 0 1 0 0 8.137E-02 2.000E-01
F 1 7 0. 0.
13 23 -1 0 1 0 0 4.647E-02 2.000E-01
F 1 7 0. 0.
14 15 -1 0 1 0 0 1.890E+00 7.000E-01
F 1 7 0. 0.
14 16 0 0 4 0 0 0.000E+00 5.000E-02
14 17 0 0 4 0 0 0.000E+00 5.000E-02
14 18 0 0 4 0 0 0.000E+00 5.000E-02
14 19 0 0 4 0 0 0.000E+00 5.000E-02
14 20 -1 0 1 0 0 1.500E-02 2.000E-01
F 1 7 0. 0.
14 21 -1 0 1 0 0 1.050E-02 2.000E-01
F 1 7 0. 0.
14 22 -1 0 1 0 0 6.400E-03 2.000E-01
F 1 7 0. 0.
14 23 -1 0 1 0 0 4.155E-03 2.000E-01
F 1 7 0. 0.
15 16 -1 0 1 0 0 1.833E+00 7.000E-01
F 1 7 0. 0.
15 17 0 0 4 0 0 0.000E+00 5.000E-02
15 18 0 0 4 0 0 0.000E+00 5.000E-02
15 19 0 0 4 0 0 0.000E+00 5.000E-02
15 20 -1 0 1 0 0 3.984E-01 2.000E-01
F 1 7 0. 0.
15 21 -1 0 1 0 0 5.632E-02 2.000E-01
F 1 7 0. 0.
15 22 -1 0 1 0 0 2.055E-02 2.000E-01
F 1 7 0. 0.
15 23 -1 0 1 0 0 1.036E-02 2.000E-01
F 1 7 0. 0.
16 17 -1 0 1 0 0 3.310E-01 7.000E-01
F 1 7 0. 0.
16 18 0 0 4 0 0 0.000E+00 5.000E-02
16 19 0 0 4 0 0 0.000E+00 5.000E-02
16 20 -1 0 1 0 0 1.156E+00 2.000E-01
F 1 7 0. 0.
16 21 -1 0 1 0 0 2.211E-01 2.000E-01
F 1 7 0. 0.
16 22 -1 0 1 0 0 9.370E-02 2.000E-01
F 1 7 0. 0.
16 23 -1 0 1 0 0 5.087E-02 2.000E-01
F 1 7 0. 0.
17 18 0 0 1 0 0 0.000E+00 7.000E-01
17 19 0 0 4 0 0 0.000E+00 5.000E-02
17 20 -1 0 1 0 0 1.926E+00 2.000E-01
F 1 7 0. 0.
17 21 -1 0 1 0 0 2.904E-01 2.000E-01
F 1 7 0. 0.
17 22 -1 0 1 0 0 1.000E-01 2.000E-01
F 1 7 0. 0.
17 23 -1 0 1 0 0 4.780E-02 2.000E-01
F 1 7 0. 0.
18 19 0 0 1 0 0 0.000E+00 7.000E-01
18 20 -1 0 1 0 0 3.673E+00 2.000E-01
F 1 7 0. 0.
18 21 -1 0 1 0 0 5.486E-01 2.000E-01
F 1 7 0. 0.
18 22 -1 0 1 0 0 1.882E-01 2.000E-01
F 1 7 0. 0.
18 23 -1 0 1 0 0 8.973E-02 2.000E-01
F 1 7 0. 0.
19 20 -1 0 1 0 0 3.673E+00 2.000E-01
F 1 7 0. 0.
19 21 -1 0 1 0 0 5.486E-01 2.000E-01
F 1 7 0. 0.
19 22 -1 0 1 0 0 1.882E-01 2.000E-01
F 1 7 0. 0.
19 23 -1 0 1 0 0 8.973E-02 2.000E-01
F 1 7 0. 0.
20 21 -1 0 1 0 0 3.282E+00 2.000E-01
F 1 7 0. 0.
20 22 -1 0 1 0 0 4.863E-01 2.000E-01
F 1 7 0. 0.
20 23 -1 0 1 0 0 1.671E-01 2.000E-01
F 1 7 0. 0.
21 22 -1 0 1 0 0 3.904E+00 2.000E-01
F 1 7 0. 0.
21 23 -1 0 1 0 0 5.676E-01 2.000E-01
F 1 7 0. 0.
22 23 -1 0 1 0 0 4.493E+00 2.000E-01
F 1 7 0. 0.
@@ -0,0 +1,149 @@
5750.0 4.50000306805 ! TEFF, GRAV
F F ! LTE, GRAY
'' ! name of non-standard flags
50 ! frequencies
99 ! NATOMS
4 1.000000e+00 0 ! H
5 8.511380e-02 0 ! He
1 1.122018e-11 0 ! Li
1 2.398833e-11 0 ! Be
1 5.011872e-10 0 ! B
5 2.454709e-04 0 ! C
5 6.025596e-05 0 ! N
5 4.570882e-04 0 ! O
1 3.630781e-08 0 ! F
1 6.918310e-05 0 ! Ne
2 1.479108e-06 0 ! Na
2 3.388442e-05 0 ! Mg
5 2.344229e-06 0 ! Al
5 3.235937e-05 0 ! Si
1 2.290868e-07 0 ! P
1 1.380384e-05 0 ! S
1 3.162278e-07 0 ! Cl
1 1.513561e-06 0 ! Ar
2 1.202264e-07 0 ! K
2 2.041738e-06 0 ! Ca
1 1.479108e-09 0 ! Sc
1 7.943282e-08 0 ! Ti
1 1.000000e-08 0 ! V
1 4.365158e-07 0 ! Cr
1 2.454709e-07 0 ! Mn
5 2.818383e-05 0 ! Fe
1 8.317638e-08 0 ! Co
1 1.698244e-06 0 ! Ni
1 1.621810e-08 0 ! Cu
1 3.981072e-08 0 ! Zn
1 7.585776e-10 0 ! Ga
1 3.801894e-09 0 ! Ge
1 1.949845e-10 0 ! As
1 2.137962e-09 0 ! Se
1 3.630781e-10 0 ! Br
1 1.778279e-09 0 ! Kr
1 3.981072e-10 0 ! Rb
1 8.317638e-10 0 ! Sr
1 1.621810e-10 0 ! Y
1 3.801894e-10 0 ! Zr
1 2.630268e-11 0 ! Nb
1 8.317638e-11 0 ! Mo
1 1.000000e-111 0 ! Tc
1 6.918310e-11 0 ! Ru
1 1.318257e-11 0 ! Rh
1 4.570882e-11 0 ! Pd
1 8.709636e-12 0 ! Ag
1 5.888437e-11 0 ! Cd
1 3.981072e-11 0 ! In
1 1.000000e-10 0 ! Sn
1 1.000000e-11 0 ! Sb
1 1.548817e-10 0 ! Te
1 3.235937e-11 0 ! I
1 1.737801e-10 0 ! Xe
1 1.174898e-11 0 ! Cs
1 1.479108e-10 0 ! Ba
1 1.348963e-11 0 ! La
1 5.011872e-11 0 ! Ce
1 3.801894e-12 0 ! Pr
1 2.818383e-11 0 ! Nd
1 1.000000e-111 0 ! Pm
1 1.000000e-11 0 ! Sm
1 3.311311e-12 0 ! Eu
1 1.288250e-11 0 ! Gd
1 1.905461e-12 0 ! Tb
1 1.380384e-11 0 ! Dy
1 3.235937e-12 0 ! Ho
1 8.511380e-12 0 ! Er
1 1.000000e-12 0 ! Tm
1 1.202264e-11 0 ! Yb
1 1.148154e-12 0 ! Lu
1 7.585776e-12 0 ! Hf
1 6.760830e-13 0 ! Ta
1 1.288250e-11 0 ! W
1 1.698244e-12 0 ! Re
1 1.778279e-11 0 ! Os
1 2.398833e-11 0 ! Ir
1 4.365158e-11 0 ! Pt
1 1.023293e-11 0 ! Au
1 1.348963e-11 0 ! Hg
1 7.943282e-12 0 ! Tl
1 1.000000e-10 0 ! Pb
1 4.466836e-12 0 ! Bi
1 1.000000e-111 0 ! Po
1 1.000000e-111 0 ! At
1 1.000000e-111 0 ! Rn
1 1.000000e-111 0 ! Fr
1 1.000000e-111 0 ! Ra
1 1.000000e-111 0 ! Ac
1 1.148154e-12 0 ! Th
1 1.000000e-111 0 ! Pa
1 3.019952e-13 0 ! U
1 1.000000e-111 0 ! Np
1 1.000000e-111 0 ! Pu
1 1.000000e-111 0 ! Am
1 1.000000e-111 0 ! Cm
1 1.000000e-111 0 ! Bk
1 1.000000e-111 0 ! Cf
1 1.000000e-111 0 ! Es
*
*
*
*
*
*
* ../data for ions
1 -1 1 0 0 1 ' H 0' 'data/hm.dat'
0 0 3 0
1 0 16 0 0 0 ' H 1' 'data/h1_16lev2.dat'
1 1 1 1 0 0 ' H 2' ' '
11 0 42 0 0 0 'Na 1' 'data/NaIkas.tl'
11 1 1 1 0 0 'Na 2' ''
12 0 96 0 0 0 'Mg 1' 'data/Mg1kas_F_ccc.sy'
12 1 29 0 0 0 'Mg 2' 'data/Mg2kas_F_ccc.sy'
12 2 1 1 0 0 'Mg 3' ' '
19 0 31 0 0 0 'K 1' 'data/KIkas.tl'
19 1 1 1 0 0 'K 2' ''
20 0 66 0 0 0 'Ca 1' 'data/Ca1kas_F_zat.sy'
20 1 24 0 0 0 'Ca 2' 'data/Ca2kas_F_zat.sy'
20 2 1 1 0 0 'Ca 3' ' '
2 0 14 0 0 0 'He 1' 'data/he1.dat'
2 1 14 0 0 0 'He 2' 'data/he2.dat '
2 2 1 1 0 0 'He 3' ' '
6 0 104 0 0 0 ' C 1' 'data/c1.t'
6 1 40 0 0 0 ' C 2' 'data/c2.t'
6 2 1 1 0 0 ' C 3' ' '
7 0 89 0 0 0 ' N 1' 'data/n1.t'
7 1 51 0 0 0 ' N 2' 'data/n2.t'
7 2 1 1 0 0 ' N 3' ' '
8 0 54 0 0 0 ' O 1' 'data/o1.t'
8 1 74 0 0 0 ' O 2' 'data/o2.t'
8 2 1 1 0 0 ' O 3' ' '
13 0 33 0 0 0 'Al 1' 'data/al1.t'
13 1 81 0 0 0 'Al 2' 'data/al2.t'
13 2 1 1 0 0 'Al 3' ' '
14 0 57 0 0 0 'Si 1' 'data/si1.t'
14 1 46 0 0 0 'Si 2' 'data/si2.t'
14 2 1 1 0 0 'Si 3' ' '
26 0 49 0 0 0 'Fe 1' 'data/tlusty_fe1_topmod.dat'
26 1 41 0 0 0 'Fe 2' 'data/tlusty_fe2_topmod.dat'
26 2 1 1 0 0 'Fe 3' ' '
0 0 0 -1 0 0 ' ' ' '
*
* end
+145
View File
@@ -0,0 +1,145 @@
5777.0 4.439995473953808 ! TEFF, GRAV
T F ! LTE, GRAY
't-msunflags' ! name of non-standard flags
50 ! frequencies
99 ! NATOMS
2 1.000000e+00 0 ! H
2 8.511380e-02 0 ! He
1 1.122018e-11 0 ! Li
1 2.398833e-11 0 ! Be
1 5.011872e-10 0 ! B
2 2.454709e-04 0 ! C
2 6.025596e-05 0 ! N
2 4.570882e-04 0 ! O
1 3.630781e-08 0 ! F
1 6.918310e-05 0 ! Ne
2 1.479108e-06 0 ! Na
2 3.388442e-05 0 ! Mg
2 2.344229e-06 0 ! Al
2 3.235937e-05 0 ! Si
1 2.290868e-07 0 ! P
1 1.380384e-05 0 ! S
1 3.162278e-07 0 ! Cl
1 1.513561e-06 0 ! Ar
1 1.202264e-07 0 ! K
2 2.041738e-06 0 ! Ca
1 1.479108e-09 0 ! Sc
1 7.943282e-08 0 ! Ti
1 1.000000e-08 0 ! V
1 4.365158e-07 0 ! Cr
1 2.454709e-07 0 ! Mn
2 2.818383e-05 0 ! Fe
1 8.317638e-08 0 ! Co
1 1.698244e-06 0 ! Ni
1 1.621810e-08 0 ! Cu
1 3.981072e-08 0 ! Zn
1 7.585776e-10 0 ! Ga
1 3.801894e-09 0 ! Ge
1 1.949845e-10 0 ! As
1 2.137962e-09 0 ! Se
1 3.630781e-10 0 ! Br
1 1.778279e-09 0 ! Kr
1 3.981072e-10 0 ! Rb
1 8.317638e-10 0 ! Sr
1 1.621810e-10 0 ! Y
1 3.801894e-10 0 ! Zr
1 2.630268e-11 0 ! Nb
1 8.317638e-11 0 ! Mo
1 1.000000e-111 0 ! Tc
1 6.918310e-11 0 ! Ru
1 1.318257e-11 0 ! Rh
1 4.570882e-11 0 ! Pd
1 8.709636e-12 0 ! Ag
1 5.888437e-11 0 ! Cd
1 3.981072e-11 0 ! In
1 1.000000e-10 0 ! Sn
1 1.000000e-11 0 ! Sb
1 1.548817e-10 0 ! Te
1 3.235937e-11 0 ! I
1 1.737801e-10 0 ! Xe
1 1.174898e-11 0 ! Cs
1 1.479108e-10 0 ! Ba
1 1.348963e-11 0 ! La
1 5.011872e-11 0 ! Ce
1 3.801894e-12 0 ! Pr
1 2.818383e-11 0 ! Nd
1 1.000000e-111 0 ! Pm
1 1.000000e-11 0 ! Sm
1 3.311311e-12 0 ! Eu
1 1.288250e-11 0 ! Gd
1 1.905461e-12 0 ! Tb
1 1.380384e-11 0 ! Dy
1 3.235937e-12 0 ! Ho
1 8.511380e-12 0 ! Er
1 1.000000e-12 0 ! Tm
1 1.202264e-11 0 ! Yb
1 1.148154e-12 0 ! Lu
1 7.585776e-12 0 ! Hf
1 6.760830e-13 0 ! Ta
1 1.288250e-11 0 ! W
1 1.698244e-12 0 ! Re
1 1.778279e-11 0 ! Os
1 2.398833e-11 0 ! Ir
1 4.365158e-11 0 ! Pt
1 1.023293e-11 0 ! Au
1 1.348963e-11 0 ! Hg
1 7.943282e-12 0 ! Tl
1 1.000000e-10 0 ! Pb
1 4.466836e-12 0 ! Bi
1 1.000000e-111 0 ! Po
1 1.000000e-111 0 ! At
1 1.000000e-111 0 ! Rn
1 1.000000e-111 0 ! Fr
1 1.000000e-111 0 ! Ra
1 1.000000e-111 0 ! Ac
1 1.148154e-12 0 ! Th
1 1.000000e-111 0 ! Pa
1 3.019952e-13 0 ! U
1 1.000000e-111 0 ! Np
1 1.000000e-111 0 ! Pu
1 1.000000e-111 0 ! Am
1 1.000000e-111 0 ! Cm
1 1.000000e-111 0 ! Bk
1 1.000000e-111 0 ! Cf
1 1.000000e-111 0 ! Es
*
*
*
* ../data for ions
1 -1 1 0 0 1 ' H 1' 'data/hm.dat'
0 0 3 0
1 0 9 0 0 0 ' H 1' 'data/h1s.dat'
1 1 1 1 0 0 ' H 2' ' '
2 0 14 0 0 0 'He 1' 'data/he1.dat'
2 1 14 0 0 0 'He 2' 'data/he2.dat '
2 2 1 1 0 0 'He 3' ' '
6 0 104 0 0 0 ' C 1' 'data/c1.t'
6 1 40 0 0 0 ' C 2' 'data/c2.t'
6 2 1 1 0 0 ' C 3' ' '
7 0 89 0 0 0 ' N 1' 'data/n1.t'
7 1 51 0 0 0 ' N 2' 'data/n2.t'
7 2 1 1 0 0 ' N 3' ' '
8 0 54 0 0 0 ' O 1' 'data/o1.t'
8 1 74 0 0 0 ' O 2' 'data/o2.t'
8 2 1 1 0 0 ' O 3' ' '
11 0 32 0 0 0 'Na 1' 'data/na1.t'
11 1 8 0 0 0 'Na 2' 'data/na2.t'
11 2 1 1 0 0 'Na 3' ' '
12 0 71 0 0 0 'Mg 1' 'data/mg1.t'
12 1 31 0 0 0 'Mg 2' 'data/mg2.t'
12 2 1 1 0 0 'Mg 3' ' '
13 0 33 0 0 0 'Al 1' 'data/al1.t'
13 1 81 0 0 0 'Al 2' 'data/al2.t'
13 2 1 1 0 0 'Al 3' ' '
14 0 57 0 0 0 'Si 1' 'data/si1.t'
14 1 46 0 0 0 'Si 2' 'data/si2.t'
14 2 1 1 0 0 'Si 3' ' '
20 0 79 0 0 0 'Ca 1' 'data/ca1.t'
20 1 32 0 0 0 'Ca 2' 'data/ca2.t'
20 2 1 1 0 0 'Ca 3' ' '
26 0 49 0 0 0 'Fe 1' 'data/tlusty_fe1_topmod.dat'
26 1 41 0 0 0 'Fe 2' 'data/tlusty_fe2_topmod.dat'
26 2 1 1 0 0 'Fe 3' ' '
0 0 0 -1 0 0 ' ' ' '
*
* end
+58
View File
@@ -0,0 +1,58 @@
56 -4
9.747804e-03 1.261161e-02 1.628152e-02 2.100596e-02 2.708258e-02 3.489451e-02 4.493235e-02 5.782370e-02 7.437161e-02 9.560419e-02 1.228361e-01 1.392096e-01 1.577464e-01 1.787304e-01 2.024826e-01 2.293656e-01 2.597912e-01 2.942231e-01 3.331833e-01 3.772637e-01 4.271308e-01 4.835414e-01 5.473434e-01 6.194854e-01 7.010383e-01 7.932117e-01 8.973545e-01 1.014975e+00 1.147741e+00 1.297527e+00 1.466367e+00 1.656400e+00 1.869780e+00 2.108407e+00 2.373490e+00 2.664780e+00 2.979596e+00 3.311843e+00 3.651890e+00 3.987931e+00 4.308212e+00 4.602781e+00 4.865205e+00 5.089970e+00 5.273269e+00 5.423154e+00 5.554118e+00 5.675944e+00 5.794678e+00 5.914327e+00 6.037798e+00 6.305785e+00 6.615138e+00 6.980588e+00 7.418741e+00 7.949527e+00
4066.800049 3.770674e+10 1.001000e-09 4.721832e+14
4102.600098 4.820083e+10 1.285000e-09 6.061491e+14
4145.899902 6.170962e+10 1.643000e-09 7.750218e+14
4190.399902 7.897992e+10 2.099000e-09 9.901225e+14
4235.500000 1.009872e+11 2.679000e-09 1.263715e+15
4280.799805 1.289719e+11 3.417000e-09 1.611839e+15
4326.100098 1.645582e+11 4.355000e-09 2.054304e+15
4371.299805 2.097848e+11 5.548000e-09 2.617056e+15
4416.299805 2.670219e+11 7.065000e-09 3.332643e+15
4461.000000 3.396882e+11 8.992000e-09 4.241631e+15
4504.899902 4.314064e+11 1.144000e-08 5.396380e+15
4527.399902 4.862200e+11 1.290000e-08 6.085079e+15
4549.500000 5.477038e+11 1.455000e-08 6.863403e+15
4571.500000 6.170043e+11 1.641000e-08 7.734681e+15
4593.500000 6.947872e+11 1.850000e-08 8.719779e+15
4615.600098 7.821695e+11 2.086000e-08 9.832139e+15
4637.799805 8.804142e+11 2.352000e-08 1.108590e+16
4660.200195 9.910482e+11 2.651000e-08 1.249520e+16
4682.899902 1.115403e+12 2.987000e-08 1.407890e+16
4706.000000 1.255537e+12 3.366000e-08 1.586528e+16
4729.899902 1.413516e+12 3.792000e-08 1.787318e+16
4754.700195 1.592004e+12 4.270000e-08 2.012618e+16
4780.899902 1.793879e+12 4.807000e-08 2.265727e+16
4808.600098 2.023058e+12 5.410000e-08 2.549945e+16
4838.299805 2.283116e+12 6.085000e-08 2.868100e+16
4870.500000 2.580340e+12 6.840000e-08 3.223963e+16
4905.899902 2.921986e+12 7.682000e-08 3.620833e+16
4944.100098 3.312564e+12 8.622000e-08 4.063896e+16
4988.100098 3.768367e+12 9.664000e-08 4.555038e+16
5034.399902 4.291969e+12 1.082000e-07 5.099915e+16
5088.600098 4.915291e+12 1.210000e-07 5.703244e+16
5148.500000 5.651609e+12 1.351000e-07 6.367853e+16
5216.799805 6.545403e+12 1.505000e-07 7.093747e+16
5294.399902 7.653441e+12 1.673000e-07 7.885646e+16
5382.500000 9.066372e+12 1.852000e-07 8.729417e+16
5483.100098 1.094768e+13 2.041000e-07 9.620366e+16
5597.100098 1.354985e+13 2.235000e-07 1.053495e+17
5727.399902 1.735192e+13 2.428000e-07 1.144494e+17
5875.700195 2.310261e+13 2.609000e-07 1.230828e+17
6044.299805 3.211736e+13 2.770000e-07 1.306858e+17
6235.200195 4.653841e+13 2.900000e-07 1.368320e+17
6451.899902 7.021360e+13 2.994000e-07 1.412894e+17
6694.799805 1.092785e+14 3.049000e-07 1.440362e+17
6983.299805 1.788247e+14 3.056000e-07 1.444362e+17
7314.799805 3.018308e+14 3.020000e-07 1.429725e+17
7618.200195 4.705612e+14 2.978000e-07 1.413799e+17
7876.899902 6.708431e+14 2.946000e-07 1.402871e+17
8097.700195 8.938029e+14 2.923000e-07 1.396401e+17
8290.400391 1.135845e+15 2.910000e-07 1.394849e+17
8462.599609 1.396051e+15 2.904000e-07 1.396799e+17
8620.200195 1.675555e+15 2.905000e-07 1.403384e+17
8903.799805 2.299047e+15 2.924000e-07 1.424285e+17
9168.500000 3.048000e+15 2.964000e-07 1.458962e+17
9424.599609 3.958947e+15 3.026000e-07 1.506232e+17
9678.400391 5.083292e+15 3.110000e-07 1.568032e+17
9934.299805 6.483555e+15 3.222000e-07 1.648308e+17
+1
View File
@@ -0,0 +1 @@
VTB= 1.0
@@ -0,0 +1,97 @@
TEFF 3500. GRAVITY 0.00000 LTE
TITLE [-0.5a] N(He)/Ntot=0.0784 VTURB=2.0 L/H=1.25 ODFNEW
OPACITY IFOP 1 1 1 1 1 1 1 1 1 1 1 1 1 0 1 0 0 0 0 0
CONVECTION ON 1.25 TURBULENCE OFF 0.00 0.00 0.00 0.00
ABUNDANCE SCALE 0.31622 ABUNDANCE CHANGE 1 0.92080 2 0.07838
ABUNDANCE CHANGE 3 -10.94 4 -10.64 5 -9.49 6 -3.52 7 -4.12 8 -2.81
ABUNDANCE CHANGE 9 -7.48 10 -3.56 11 -5.71 12 -4.06 13 -5.57 14 -4.09
ABUNDANCE CHANGE 15 -6.59 16 -4.31 17 -6.54 18 -5.24 19 -6.92 20 -5.28
ABUNDANCE CHANGE 21 -8.87 22 -6.62 23 -8.04 24 -6.37 25 -6.65 26 -4.54
ABUNDANCE CHANGE 27 -7.12 28 -5.79 29 -7.83 30 -7.44 31 -9.16 32 -8.63
ABUNDANCE CHANGE 33 -9.67 34 -8.63 35 -9.41 36 -8.73 37 -9.44 38 -9.07
ABUNDANCE CHANGE 39 -9.80 40 -9.44 41 -10.62 42 -10.12 43 -20.00 44 -10.20
ABUNDANCE CHANGE 45 -10.92 46 -10.35 47 -11.10 48 -10.27 49 -10.38 50 -10.04
ABUNDANCE CHANGE 51 -11.04 52 -9.80 53 -10.53 54 -9.87 55 -10.91 56 -9.91
ABUNDANCE CHANGE 57 -10.87 58 -10.46 59 -11.33 60 -10.54 61 -20.00 62 -11.03
ABUNDANCE CHANGE 63 -11.53 64 -10.92 65 -11.69 66 -10.90 67 -11.78 68 -11.11
ABUNDANCE CHANGE 69 -12.04 70 -10.96 71 -11.98 72 -11.16 73 -12.17 74 -10.93
ABUNDANCE CHANGE 75 -11.76 76 -10.59 77 -10.69 78 -10.24 79 -11.03 80 -10.91
ABUNDANCE CHANGE 81 -11.14 82 -10.09 83 -11.33 84 -20.00 85 -20.00 86 -20.00
ABUNDANCE CHANGE 87 -20.00 88 -20.00 89 -20.00 90 -11.95 91 -20.00 92 -12.54
ABUNDANCE CHANGE 93 -20.00 94 -20.00 95 -20.00 96 -20.00 97 -20.00 98 -20.00
ABUNDANCE CHANGE 99 -20.00
READ DECK6 72 RHOX,T,P,XNE,ABROSS,ACCRAD,VTURB, FLXCNV,VCONV,VELSND
9.95014062E-03 2113.7 9.931E-03 1.058E+05 1.340E-05 2.028E-03 2.000E+05 0.000E+00 0.000E+00 2.449E+06
1.31458396E-02 2131.0 1.312E-02 1.393E+05 1.443E-05 1.872E-03 2.000E+05 0.000E+00 0.000E+00 2.139E+06
1.71534204E-02 2149.0 1.712E-02 1.816E+05 1.517E-05 1.732E-03 2.000E+05 0.000E+00 0.000E+00 1.887E+06
2.23196810E-02 2169.0 2.228E-02 2.367E+05 1.545E-05 1.599E-03 2.000E+05 0.000E+00 0.000E+00 1.675E+06
2.91547521E-02 2191.2 2.910E-02 3.109E+05 1.541E-05 1.468E-03 2.000E+05 0.000E+00 0.000E+00 1.492E+06
3.79641312E-02 2209.6 3.790E-02 4.047E+05 1.652E-05 1.327E-03 2.000E+05 0.000E+00 0.000E+00 1.326E+06
4.89343670E-02 2227.9 4.886E-02 5.219E+05 1.761E-05 1.205E-03 2.000E+05 0.000E+00 0.000E+00 1.190E+06
6.28094373E-02 2247.2 6.272E-02 6.717E+05 1.835E-05 1.102E-03 2.000E+05 0.000E+00 0.000E+00 1.075E+06
8.07811629E-02 2267.8 8.067E-02 8.683E+05 1.870E-05 1.013E-03 2.000E+05 0.000E+00 0.000E+00 9.774E+05
1.04533817E-01 2290.1 1.044E-01 1.132E+06 1.875E-05 9.320E-04 2.000E+05 0.000E+00 0.000E+00 8.926E+05
1.34847526E-01 2309.5 1.347E-01 1.464E+06 2.038E-05 8.438E-04 2.000E+05 0.000E+00 0.000E+00 8.183E+05
1.72289107E-01 2328.7 1.721E-01 1.877E+06 2.177E-05 7.727E-04 2.000E+05 0.000E+00 0.000E+00 7.583E+05
2.19448610E-01 2348.2 2.192E-01 2.401E+06 2.286E-05 7.138E-04 2.000E+05 0.000E+00 0.000E+00 7.089E+05
2.80027992E-01 2368.5 2.798E-01 3.081E+06 2.357E-05 6.639E-04 2.000E+05 0.000E+00 0.000E+00 6.676E+05
3.58047990E-01 2388.9 3.577E-01 3.962E+06 2.451E-05 6.194E-04 2.000E+05 0.000E+00 0.000E+00 6.332E+05
4.56409344E-01 2409.2 4.560E-01 5.078E+06 2.635E-05 5.760E-04 2.000E+05 0.000E+00 0.000E+00 6.052E+05
5.77905734E-01 2428.6 5.775E-01 6.458E+06 2.853E-05 5.386E-04 2.000E+05 0.000E+00 0.000E+00 5.829E+05
7.28413455E-01 2447.8 7.279E-01 8.177E+06 3.046E-05 5.080E-04 2.000E+05 0.000E+00 0.000E+00 5.652E+05
9.18113689E-01 2467.4 9.175E-01 1.036E+07 3.207E-05 4.815E-04 2.000E+05 0.000E+00 0.000E+00 5.510E+05
1.15654779E+00 2486.6 1.156E+00 1.310E+07 3.427E-05 4.575E-04 2.000E+05 0.000E+00 0.000E+00 5.395E+05
1.45336012E+00 2506.4 1.453E+00 1.655E+07 3.679E-05 4.349E-04 2.000E+05 0.000E+00 0.000E+00 5.307E+05
1.81960140E+00 2526.5 1.819E+00 2.086E+07 4.001E-05 4.123E-04 2.000E+05 0.000E+00 0.000E+00 5.241E+05
2.26873126E+00 2546.2 2.268E+00 2.617E+07 4.339E-05 3.923E-04 2.000E+05 0.000E+00 0.000E+00 5.189E+05
2.82493371E+00 2565.9 2.824E+00 3.278E+07 4.651E-05 3.740E-04 2.000E+05 0.000E+00 0.000E+00 5.150E+05
3.51423165E+00 2585.3 3.513E+00 4.097E+07 5.026E-05 3.578E-04 2.000E+05 0.000E+00 0.000E+00 5.118E+05
4.35991527E+00 2604.7 4.358E+00 5.109E+07 5.492E-05 3.431E-04 2.000E+05 0.000E+00 0.000E+00 5.095E+05
5.39817138E+00 2625.4 5.396E+00 6.381E+07 5.931E-05 3.271E-04 2.000E+05 0.000E+00 0.000E+00 5.082E+05
6.66906743E+00 2646.1 6.667E+00 7.952E+07 6.513E-05 3.138E-04 2.000E+05 0.000E+00 0.000E+00 5.074E+05
8.21285186E+00 2666.6 8.210E+00 9.872E+07 7.131E-05 3.021E-04 2.000E+05 0.000E+00 0.000E+00 5.069E+05
1.01058416E+01 2687.4 1.010E+01 1.226E+08 7.726E-05 2.898E-04 2.000E+05 0.000E+00 0.000E+00 5.068E+05
1.24132488E+01 2708.2 1.241E+01 1.519E+08 8.526E-05 2.789E-04 2.000E+05 0.000E+00 0.000E+00 5.069E+05
1.52167353E+01 2730.5 1.521E+01 1.887E+08 9.288E-05 2.651E-04 2.000E+05 0.000E+00 0.000E+00 5.077E+05
1.86567964E+01 2753.5 1.865E+01 2.347E+08 1.010E-04 2.520E-04 2.000E+05 0.000E+00 0.000E+00 5.087E+05
2.28264349E+01 2775.9 2.282E+01 2.909E+08 1.123E-04 2.449E-04 2.000E+05 0.000E+00 0.000E+00 5.096E+05
2.78734624E+01 2800.0 2.787E+01 3.617E+08 1.227E-04 2.332E-04 2.000E+05 0.000E+00 0.000E+00 5.112E+05
3.39091438E+01 2817.1 3.391E+01 4.385E+08 1.394E-04 2.383E-04 2.000E+05 0.000E+00 0.000E+00 5.107E+05
4.11744312E+01 2843.7 4.117E+01 5.464E+08 1.510E-04 2.253E-04 2.000E+05 0.000E+00 0.000E+00 5.131E+05
5.00665232E+01 2869.2 5.006E+01 6.789E+08 1.653E-04 2.159E-04 2.000E+05 0.000E+00 0.000E+00 5.150E+05
6.08526094E+01 2895.5 6.084E+01 8.447E+08 1.825E-04 2.096E-04 2.000E+05 0.000E+00 0.000E+00 5.172E+05
7.38161765E+01 2921.6 7.380E+01 1.048E+09 2.034E-04 2.074E-04 2.000E+05 0.000E+00 0.000E+00 5.193E+05
8.94287919E+01 2949.5 8.941E+01 1.306E+09 2.232E-04 2.037E-04 2.000E+05 0.000E+00 0.000E+00 5.219E+05
1.08497881E+02 2980.5 1.085E+02 1.643E+09 2.433E-04 1.981E-04 2.000E+05 0.000E+00 0.000E+00 5.252E+05
1.31703792E+02 3012.8 1.317E+02 2.075E+09 2.681E-04 1.953E-04 2.000E+05 0.000E+00 0.000E+00 5.287E+05
1.59406796E+02 3045.4 1.594E+02 2.614E+09 3.029E-04 2.004E-04 2.000E+05 0.000E+00 0.000E+00 5.323E+05
1.92110421E+02 3078.3 1.921E+02 3.284E+09 3.414E-04 2.088E-04 2.000E+05 0.000E+00 0.000E+00 5.359E+05
2.31130112E+02 3117.3 2.311E+02 4.194E+09 3.787E-04 2.160E-04 2.000E+05 0.000E+00 0.000E+00 5.411E+05
2.78136213E+02 3159.9 2.781E+02 5.410E+09 4.193E-04 2.256E-04 2.000E+05 0.000E+00 0.000E+00 5.470E+05
3.33511550E+02 3207.2 3.334E+02 7.047E+09 4.859E-04 2.499E-04 2.000E+05 0.000E+00 0.000E+00 5.539E+05
3.96749157E+02 3262.9 3.967E+02 9.339E+09 5.712E-04 2.825E-04 2.000E+05 0.000E+00 0.000E+00 5.626E+05
4.67527498E+02 3330.6 4.674E+02 1.267E+10 6.915E-04 3.288E-04 2.000E+05 0.000E+00 0.000E+00 5.738E+05
5.43110585E+02 3411.2 5.430E+02 1.748E+10 8.821E-04 4.016E-04 2.000E+05 0.000E+00 0.000E+00 5.870E+05
6.22977352E+02 3502.6 6.228E+02 2.418E+10 1.101E-03 4.720E-04 2.000E+05 0.000E+00 0.000E+00 6.012E+05
7.09197329E+02 3604.1 7.090E+02 3.320E+10 1.350E-03 5.303E-04 2.000E+05 0.000E+00 0.000E+00 6.154E+05
7.97828468E+02 3718.3 7.976E+02 4.486E+10 1.861E-03 6.803E-04 2.000E+05 0.000E+00 0.000E+00 6.297E+05
8.83007392E+02 3843.4 8.827E+02 5.865E+10 2.542E-03 8.858E-04 2.000E+05 0.000E+00 0.000E+00 6.434E+05
9.70825313E+02 3988.6 9.704E+02 7.509E+10 3.136E-03 1.009E-03 2.000E+05 8.781E-15 1.349E+01 6.576E+05
1.06846597E+03 4141.7 1.068E+03 9.299E+10 3.674E-03 1.124E-03 2.000E+05 3.612E-13 4.580E+01 6.715E+05
1.18222275E+03 4320.5 1.182E+03 1.130E+11 4.138E-03 1.210E-03 2.000E+05 1.151E-12 6.628E+01 6.875E+05
1.31707445E+03 4514.7 1.316E+03 1.358E+11 4.658E-03 1.337E-03 2.000E+05 4.260E-12 1.006E+02 7.040E+05
1.47431310E+03 4740.4 1.473E+03 1.770E+11 5.464E-03 1.527E-03 2.000E+05 1.632E-10 3.318E+02 7.213E+05
1.63813170E+03 4989.0 1.637E+03 2.808E+11 7.804E-03 2.160E-03 2.000E+05 1.725E-08 1.537E+03 7.383E+05
1.77522389E+03 5275.4 1.773E+03 5.539E+11 1.367E-02 3.787E-03 2.000E+05 1.637E-06 6.909E+03 7.550E+05
1.87318282E+03 5595.9 1.871E+03 1.225E+12 2.668E-02 7.430E-03 2.000E+05 1.059E-04 2.740E+04 7.689E+05
1.93746837E+03 5958.1 1.935E+03 2.847E+12 5.571E-02 1.555E-02 2.000E+05 1.975E-03 7.129E+04 7.769E+05
1.97776871E+03 6353.6 1.974E+03 6.526E+12 1.195E-01 3.164E-02 2.000E+05 1.430E-02 1.289E+05 7.690E+05
2.00312907E+03 6746.3 1.998E+03 1.358E+13 2.466E-01 5.164E-02 2.000E+05 2.122E-01 3.044E+05 7.754E+05
2.02105852E+03 7049.0 2.015E+03 2.260E+13 4.243E-01 5.484E-02 2.000E+05 5.668E-01 4.169E+05 7.760E+05
2.03638136E+03 7254.9 2.030E+03 3.121E+13 6.118E-01 4.719E-02 2.000E+05 7.345E-01 4.339E+05 7.786E+05
2.05122943E+03 7415.4 2.044E+03 3.963E+13 8.115E-01 4.095E-02 2.000E+05 8.199E-01 4.324E+05 7.820E+05
2.06652067E+03 7552.7 2.059E+03 4.823E+13 1.031E+00 3.735E-02 2.000E+05 8.755E-01 4.374E+05 7.860E+05
2.08263897E+03 7684.8 2.074E+03 5.783E+13 1.296E+00 3.368E-02 2.000E+05 9.070E-01 4.281E+05 7.908E+05
2.10007909E+03 7797.1 2.091E+03 6.718E+13 1.572E+00 3.294E-02 2.000E+05 9.262E-01 4.263E+05 7.955E+05
PRADK 1.9910E-01
BEGIN ITERATION 15 COMPLETED
@@ -0,0 +1,97 @@
TEFF 3500. GRAVITY 5.00000 LTE
TITLE [-0.5a] N(He)/Ntot=0.0784 VTURB=2.0 L/H=1.25 ODFNEW
OPACITY IFOP 1 1 1 1 1 1 1 1 1 1 1 1 1 0 1 0 0 0 0 0
CONVECTION ON 1.25 TURBULENCE OFF 0.00 0.00 0.00 0.00
ABUNDANCE SCALE 0.31622 ABUNDANCE CHANGE 1 0.92080 2 0.07838
ABUNDANCE CHANGE 3 -10.94 4 -10.64 5 -9.49 6 -3.52 7 -4.12 8 -2.81
ABUNDANCE CHANGE 9 -7.48 10 -3.56 11 -5.71 12 -4.06 13 -5.57 14 -4.09
ABUNDANCE CHANGE 15 -6.59 16 -4.31 17 -6.54 18 -5.24 19 -6.92 20 -5.28
ABUNDANCE CHANGE 21 -8.87 22 -6.62 23 -8.04 24 -6.37 25 -6.65 26 -4.54
ABUNDANCE CHANGE 27 -7.12 28 -5.79 29 -7.83 30 -7.44 31 -9.16 32 -8.63
ABUNDANCE CHANGE 33 -9.67 34 -8.63 35 -9.41 36 -8.73 37 -9.44 38 -9.07
ABUNDANCE CHANGE 39 -9.80 40 -9.44 41 -10.62 42 -10.12 43 -20.00 44 -10.20
ABUNDANCE CHANGE 45 -10.92 46 -10.35 47 -11.10 48 -10.27 49 -10.38 50 -10.04
ABUNDANCE CHANGE 51 -11.04 52 -9.80 53 -10.53 54 -9.87 55 -10.91 56 -9.91
ABUNDANCE CHANGE 57 -10.87 58 -10.46 59 -11.33 60 -10.54 61 -20.00 62 -11.03
ABUNDANCE CHANGE 63 -11.53 64 -10.92 65 -11.69 66 -10.90 67 -11.78 68 -11.11
ABUNDANCE CHANGE 69 -12.04 70 -10.96 71 -11.98 72 -11.16 73 -12.17 74 -10.93
ABUNDANCE CHANGE 75 -11.76 76 -10.59 77 -10.69 78 -10.24 79 -11.03 80 -10.91
ABUNDANCE CHANGE 81 -11.14 82 -10.09 83 -11.33 84 -20.00 85 -20.00 86 -20.00
ABUNDANCE CHANGE 87 -20.00 88 -20.00 89 -20.00 90 -11.95 91 -20.00 92 -12.54
ABUNDANCE CHANGE 93 -20.00 94 -20.00 95 -20.00 96 -20.00 97 -20.00 98 -20.00
ABUNDANCE CHANGE 99 -20.00
READ DECK6 72 RHOX,T,P,XNE,ABROSS,ACCRAD,VTURB, FLXCNV,VCONV,VELSND
1.48528604E-04 2507.3 1.485E+01 1.135E+08 8.978E-04 9.299E-03 2.000E+05 0.000E+00 0.000E+00 4.420E+05
1.92729547E-04 2520.9 1.927E+01 1.443E+08 1.115E-03 9.760E-03 2.000E+05 0.000E+00 0.000E+00 4.406E+05
2.40588458E-04 2530.8 2.406E+01 1.765E+08 1.364E-03 1.031E-02 2.000E+05 0.000E+00 0.000E+00 4.392E+05
2.93587231E-04 2540.4 2.936E+01 2.119E+08 1.621E-03 1.086E-02 2.000E+05 0.000E+00 0.000E+00 4.382E+05
3.52734230E-04 2546.5 3.527E+01 2.493E+08 1.954E-03 1.149E-02 2.000E+05 0.000E+00 0.000E+00 4.366E+05
4.17751696E-04 2549.6 4.178E+01 2.882E+08 2.379E-03 1.226E-02 2.000E+05 0.000E+00 0.000E+00 4.347E+05
4.89225147E-04 2551.9 4.892E+01 3.295E+08 2.876E-03 1.317E-02 2.000E+05 0.000E+00 0.000E+00 4.328E+05
5.67917426E-04 2553.0 5.680E+01 3.732E+08 3.478E-03 1.428E-02 2.000E+05 0.000E+00 0.000E+00 4.308E+05
6.55496507E-04 2556.2 6.563E+01 4.226E+08 4.079E-03 1.522E-02 2.000E+05 0.000E+00 0.000E+00 4.293E+05
7.55497356E-04 2557.8 7.562E+01 4.756E+08 4.856E-03 1.640E-02 2.000E+05 0.000E+00 0.000E+00 4.275E+05
8.68422035E-04 2520.0 8.530E+01 4.932E+08 7.859E-03 2.458E-02 2.000E+05 0.000E+00 0.000E+00 4.168E+05
9.56628962E-04 2430.9 9.265E+01 4.631E+08 1.451E-02 4.659E-02 2.000E+05 0.000E+00 0.000E+00 3.927E+05
1.00262634E-03 2301.1 9.777E+01 3.871E+08 2.756E-02 9.460E-02 2.000E+05 0.000E+00 0.000E+00 3.546E+05
1.03711499E-03 2147.7 1.017E+02 2.752E+08 4.153E-02 1.220E-01 2.000E+05 0.000E+00 0.000E+00 3.155E+05
1.08238400E-03 2079.8 1.062E+02 1.765E+08 4.252E-02 1.255E-01 2.000E+05 0.000E+00 0.000E+00 3.024E+05
1.14155010E-03 2076.5 1.121E+02 1.621E+08 4.170E-02 1.254E-01 2.000E+05 0.000E+00 0.000E+00 3.014E+05
1.22116818E-03 2084.7 1.201E+02 1.751E+08 4.200E-02 1.253E-01 2.000E+05 0.000E+00 0.000E+00 3.023E+05
1.32643570E-03 2095.2 1.306E+02 1.948E+08 4.241E-02 1.249E-01 2.000E+05 0.000E+00 0.000E+00 3.035E+05
1.46556059E-03 2107.0 1.445E+02 2.205E+08 4.278E-02 1.241E-01 2.000E+05 0.000E+00 0.000E+00 3.047E+05
1.64921363E-03 2119.2 1.629E+02 2.530E+08 4.322E-02 1.234E-01 2.000E+05 0.000E+00 0.000E+00 3.059E+05
1.89154334E-03 2131.4 1.872E+02 2.934E+08 4.373E-02 1.228E-01 2.000E+05 0.000E+00 0.000E+00 3.069E+05
2.21043491E-03 2145.3 2.191E+02 3.469E+08 4.438E-02 1.222E-01 2.000E+05 0.000E+00 0.000E+00 3.081E+05
2.62870199E-03 2161.8 2.610E+02 4.193E+08 4.522E-02 1.217E-01 2.000E+05 0.000E+00 0.000E+00 3.096E+05
3.17502976E-03 2179.4 3.156E+02 5.142E+08 4.624E-02 1.213E-01 2.000E+05 0.000E+00 0.000E+00 3.111E+05
3.88988280E-03 2198.3 3.872E+02 6.385E+08 4.697E-02 1.197E-01 2.000E+05 0.000E+00 0.000E+00 3.126E+05
4.82944448E-03 2217.6 4.812E+02 8.006E+08 4.767E-02 1.178E-01 2.000E+05 0.000E+00 0.000E+00 3.141E+05
6.06040355E-03 2242.0 6.043E+02 1.031E+09 4.867E-02 1.160E-01 2.000E+05 0.000E+00 0.000E+00 3.164E+05
7.66513851E-03 2264.9 7.648E+02 1.322E+09 4.984E-02 1.146E-01 2.000E+05 0.000E+00 0.000E+00 3.182E+05
9.76709019E-03 2267.2 9.751E+02 1.571E+09 5.049E-02 1.137E-01 2.000E+05 0.000E+00 0.000E+00 3.168E+05
1.25162799E-02 2294.5 1.250E+03 2.067E+09 5.181E-02 1.122E-01 2.000E+05 0.000E+00 0.000E+00 3.192E+05
1.60877683E-02 2341.5 1.607E+03 2.920E+09 5.321E-02 1.094E-01 2.000E+05 9.858E-04 2.179E+04 3.245E+05
2.07082188E-02 2385.6 2.069E+03 4.053E+09 5.502E-02 1.075E-01 2.000E+05 6.080E-04 1.721E+04 3.294E+05
2.66842659E-02 2429.6 2.667E+03 5.591E+09 5.659E-02 1.048E-01 2.000E+05 4.808E-04 1.478E+04 3.344E+05
3.44065998E-02 2473.4 3.439E+03 7.663E+09 5.859E-02 1.029E-01 2.000E+05 4.371E-04 1.330E+04 3.392E+05
4.43601301E-02 2518.5 4.435E+03 1.049E+10 6.042E-02 1.004E-01 2.000E+05 8.986E-04 1.572E+04 3.442E+05
5.73693439E-02 2566.6 5.736E+03 1.444E+10 6.117E-02 9.569E-02 2.000E+05 5.318E-04 1.226E+04 3.497E+05
7.43339605E-02 2611.6 7.432E+03 1.967E+10 6.317E-02 9.328E-02 2.000E+05 3.853E-04 1.022E+04 3.545E+05
9.62520741E-02 2662.4 9.624E+03 2.706E+10 6.506E-02 8.998E-02 2.000E+05 2.374E-03 1.744E+04 3.603E+05
1.24727356E-01 2714.0 1.247E+04 3.717E+10 6.664E-02 8.570E-02 2.000E+05 1.758E-03 1.467E+04 3.662E+05
1.61721387E-01 2765.9 1.617E+04 5.092E+10 6.853E-02 8.158E-02 2.000E+05 2.845E-03 1.602E+04 3.719E+05
2.09971012E-01 2822.4 2.100E+04 7.031E+10 6.972E-02 7.585E-02 2.000E+05 5.837E-03 1.895E+04 3.785E+05
2.71941249E-01 2878.9 2.719E+04 9.648E+10 7.382E-02 7.347E-02 2.000E+05 5.486E-03 1.729E+04 3.849E+05
3.51227397E-01 2936.9 3.512E+04 1.319E+11 7.579E-02 6.806E-02 2.000E+05 9.959E-03 1.969E+04 3.915E+05
4.53666857E-01 2998.8 4.537E+04 1.810E+11 7.862E-02 6.292E-02 2.000E+05 1.270E-02 1.994E+04 3.987E+05
5.85567776E-01 3060.6 5.856E+04 2.470E+11 8.130E-02 5.730E-02 2.000E+05 1.484E-02 1.961E+04 4.057E+05
7.53148657E-01 3126.1 7.531E+04 3.367E+11 8.672E-02 5.354E-02 2.000E+05 2.402E-02 2.159E+04 4.133E+05
9.60373804E-01 3190.6 9.604E+04 4.530E+11 9.429E-02 5.121E-02 2.000E+05 2.430E-02 2.030E+04 4.206E+05
1.21720848E+00 3256.5 1.217E+05 6.052E+11 1.005E-01 4.719E-02 2.000E+05 3.821E-02 2.225E+04 4.282E+05
1.53532889E+00 3324.7 1.535E+05 8.055E+11 1.092E-01 4.470E-02 2.000E+05 4.322E-02 2.182E+04 4.361E+05
1.92604816E+00 3392.4 1.926E+05 1.063E+12 1.184E-01 4.254E-02 2.000E+05 5.488E-02 2.231E+04 4.437E+05
2.39783186E+00 3463.0 2.398E+05 1.398E+12 1.330E-01 4.332E-02 2.000E+05 7.941E-02 2.398E+04 4.518E+05
3.02191652E+00 3540.0 3.022E+05 1.869E+12 1.205E-01 3.428E-02 2.000E+05 8.005E-02 2.253E+04 4.606E+05
3.95074004E+00 3634.2 3.951E+05 2.632E+12 1.091E-01 3.114E-02 2.000E+05 1.394E-01 2.558E+04 4.714E+05
5.01121003E+00 3722.7 5.011E+05 3.592E+12 1.590E-01 3.839E-02 2.000E+05 2.000E-01 2.719E+04 4.814E+05
6.01312121E+00 3794.6 6.013E+05 4.588E+12 2.153E-01 4.377E-02 2.000E+05 2.917E-01 2.967E+04 4.896E+05
7.09788466E+00 3865.1 7.098E+05 5.781E+12 2.455E-01 4.275E-02 2.000E+05 3.786E-01 3.111E+04 4.977E+05
8.36754798E+00 3937.0 8.368E+05 7.295E+12 2.798E-01 4.086E-02 2.000E+05 4.765E-01 3.239E+04 5.059E+05
9.84184023E+00 4013.0 9.842E+05 9.253E+12 3.235E-01 3.822E-02 2.000E+05 5.828E-01 3.373E+04 5.146E+05
1.15444513E+01 4090.0 1.154E+06 1.173E+13 3.732E-01 3.470E-02 2.000E+05 6.533E-01 3.338E+04 5.233E+05
1.34922408E+01 4169.7 1.349E+06 1.488E+13 4.407E-01 3.162E-02 2.000E+05 7.468E-01 3.467E+04 5.323E+05
1.56744106E+01 4250.0 1.567E+06 1.879E+13 5.279E-01 2.897E-02 2.000E+05 7.809E-01 3.303E+04 5.414E+05
1.80945321E+01 4329.4 1.809E+06 2.355E+13 6.371E-01 2.733E-02 2.000E+05 8.459E-01 3.429E+04 5.503E+05
2.07464365E+01 4411.2 2.075E+06 2.940E+13 7.802E-01 2.590E-02 2.000E+05 8.648E-01 3.235E+04 5.595E+05
2.36402598E+01 4489.4 2.364E+06 3.624E+13 9.513E-01 2.507E-02 2.000E+05 9.056E-01 3.329E+04 5.680E+05
2.67957132E+01 4573.0 2.680E+06 4.472E+13 1.163E+00 2.433E-02 2.000E+05 9.202E-01 3.185E+04 5.774E+05
3.02885452E+01 4653.2 3.029E+06 5.461E+13 1.384E+00 2.357E-02 2.000E+05 9.395E-01 3.193E+04 5.861E+05
3.41882596E+01 4742.9 3.419E+06 6.725E+13 1.660E+00 2.323E-02 2.000E+05 9.504E-01 3.137E+04 5.961E+05
3.85379980E+01 4829.9 3.854E+06 8.203E+13 1.980E+00 2.281E-02 2.000E+05 9.584E-01 3.059E+04 6.056E+05
4.33757224E+01 4927.3 4.338E+06 1.008E+14 2.382E+00 2.295E-02 2.000E+05 9.670E-01 3.071E+04 6.164E+05
4.87669685E+01 5023.5 4.877E+06 1.229E+14 2.837E+00 2.285E-02 2.000E+05 9.708E-01 2.966E+04 6.268E+05
5.47952042E+01 5131.3 5.480E+06 1.509E+14 3.388E+00 2.322E-02 2.000E+05 9.763E-01 2.981E+04 6.387E+05
6.15531214E+01 5240.5 6.155E+06 1.843E+14 4.014E+00 2.420E-02 2.000E+05 9.783E-01 2.921E+04 6.506E+05
PRADK 1.9805E-01
BEGIN ITERATION 15 COMPLETED
+24
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import setuptools
import synple
with open("README.md", "r") as fh:
long_description = fh.read()
setuptools.setup(
name="synple", # Replace with your own username
version="0.2",
author="Carlos Allende Prieto",
author_email="callende@iac.es",
description="A simple package to compute synthetic stellar spectra",
long_description=long_description,
long_description_content_type="text/markdown",
url="https://github.com/callendeprieto/synple",
packages=setuptools.find_packages(),
classifiers=[
"Programming Language :: Python :: 3",
"License :: OSI Approved :: MIT License",
"Operating System :: OS Independent",
],
python_requires='>=3.6',
)
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PARAMETER (MLIN0 =1200000,
* MGRIEM = 10,
* MNLT = 2000,
* MSPHE2 = 20,
* MLIN = 400000,
* MPRF = MLIN0)
C
PARAMETER (MLINM0 =9000000,
* MLINM =2000000,
* MMLIST = 3)
C
REAL*4 EXCL0(MLIN0),
* EXCU0(MLIN0),
* GF0(MLIN0),
* EXTIN(MLIN0),
* BNUL(MLIN0),
* GAMR0(MPRF),
* GS0(MPRF),
* GW0(MPRF),
* WGR0(4,MGRIEM),
* EXCLM(MLINM0,MMLIST),
* GFM(MLINM0,MMLIST),
* EXTINM(MLINM0,MMLIST),
* GRM(MLINM0,MMLIST),
* GSM(MLINM0,MMLIST),
* GWM(MLINM0,MMLIST),
* GVDWH2(MLINM0,MMLIST),
* GEXPH2(MLINM0,MMLIST),
* GVDWHE(MLINM0,MMLIST),
* GEXPHE(MLINM0,MMLIST)
C
COMMON/LINTOT/FREQ0(MLIN0),
* EXCL0,
* EXCU0,
* GF0,
* EXTIN,
* BNUL,
* INDAT(MLIN0),
* INDNLT(MLIN0),
* ILOWN(MLIN0),
* IUPN(MLIN0),
* IJCONT(MLIN0),
* INDLIN(MLIN),
* INDLIP(MLIN),
* NLIN0,NLIN,IRLIST,
* NNLT,NGRIEM
C
COMMON/MOLTOT/FREQM(MLINM0,MMLIST),
* EXCLM,
* GFM,
* EXTINM,
* GRM,GSM,GWM,
* GVDWH2,GEXPH2,GVDWHE,GEXPHE,
* INDATM(MLINM0,MMLIST),
* INMLIN(MLINM,MMLIST),
* INMLIP(MLINM,MMLIST),
* NLINM0(MMLIST),
* NLINML(MMLIST),
* NLINMT(MMLIST),
* IUNITM(MMLIST),
* INACTM(MMLIST),
* IVDWLI(MMLIST),
* NMLIST
CHARACTER*40 AMLIST(0:MMLIST)
COMMON/LISPAR/AMLIST,
* IBIN(0:MMLIST)
C
COMMON/LINPRF/GAMR0,
* GS0,
* GW0,
* WGR0,
* IPRF0(MPRF),
* ISPRF(MPRF),
* IGRIEM(MPRF),
* ISP0(MSPHE2),NSP
C
COMMON/LINNLT/ABCENT(MNLT,MDEPTH),
* SLIN(MNLT,MDEPTH)
C
COMMON/LINDEP/PLAN(MDEPTH),
* STIM(MDEPTH),
* EXHK(MDEPTH)
C
COMMON/LINCTR/DFRCON,IJCNTR(MLIN),IJCMTR(MLINM,MMLIST)
COMMON/MLINRE/FRLASM(MMLIST),ALASTM(MMLIST),TMLIM(MMLIST),
* NXTSEM(MMLIST),IPRSEM(MMLIST),IREADM(MMLIST)
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C
C Basic parameters of the model atmosphere
C
COMMON/MODELP/DM(MDEPTH),
* TEMP(MDEPTH),
* ELEC(MDEPTH),
* DENS(MDEPTH),
* ZD(MDEPTH),
* VTURB(MDEPTH),VTB,
* ABSTD(MDEPTH),
* ABSTDW(MFREQC,MDEPTH),
* POPUL(MLEVEL,MDEPTH),
* POPREL(MLEVEL,MDEPTH),
* DMR0(MDEPTH),
* DMRP(MDEPTH),
* SBF(MLEVEL),
* USUM(MIOEX),
* WOP(MLEVEL,MDEPTH),
* WNHINT(NLMX,MDEPTH),
* WNHE2(NLMX,MDEPTH),
* RRR(MDEPTH,MION,MATOM),
* JT(MDEPTH),
* TI0(MDEPTH),
* TI1(MDEPTH),
* TI2(MDEPTH)
character*8 cmol(mmolec)
COMMON/MOLPAR/RRMOL(MMOLEC,MDEPTH),
* DOPMOL(MMOLEC,MDEPTH),
* AMMOL(MMOLEC),
* CMOL,
* anh2(mdepth),anch(mdepth),anoh(mdepth),
* anhm(mdepth)
C
COMMON/OPACAT/OPATM(MATOM,MFREQ,MDEPTH),
* EMATM(MATOM,MFREQ,MDEPTH),
* OPATML(MATOM,MFREQ),
* GRADAT(MATOM,MDEPTH),
* GRADFA(MATOM,MDEPTH),
* POPAT(MATOM,MDEPTH),
* DGRAD0(MATOM,MATOM,MDEPTH),
* DGRADP(MATOM,MATOM,MDEPTH)
C
COMMON/RADFLD/RAD(MFREQ,MDEPTH),
c * FAK(MFREQ,MDEPTH),
c * ALI(MFREQ,MDEPTH),
c * FLXH(MFREQ,MDEPTH),
* RAD0(MFREQ,MDEPTH),
* FLX0(MFREQ,MDEPTH),
* flxt(mdepth),
* flxi(mdepth)
C
COMMON/XENPRF/PRFXB(MLINH,MHWL,MHT,MHE),
* PRFXR(MLINH,MHWL,MHT,MHE),
* PRFB(MLINH,MDEPTH,MHWL),
* PRFR(MLINH,MDEPTH,MHWL),
* ALXEN(MLINH,MHWL),
* XTXEN(MHT,MLINH),
* XNEXEN(MHE,MLINH),XNEMIN,
* NWLXEN(MLINH),
* NTHXEN(MLINH),
* NEHXEN(MLINH),
* ILXEN(4,22),
* IHXENB
C
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PARAMETER (MFRTAB = 100000,
* MTTAB = 20,
* MRTAB = 20,
* MSFTAB = 2000000.
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C
C Parameters that specify dimensions of arrays
C
IMPLICIT REAL*8 (A-H, O-Z),LOGICAL*1 (L)
character*4 typat
PARAMETER (MATEX = 30,
* MIOEX = 90,
* MLEVEL= 1650,
* MDEPTH= 100,
* MDEPF = 500,
* MFREQ = 2000,
c * MFREQ = 120,
* MFREQC= 2000,
* MFRQ = 2000,
* MOPAC = MFRQ,
* MMU = 20,
* MCROSS= MLEVEL,
* MFIT = 1650,
* MFCRA = 1200,
* MTRAD = 3,
* MATOM = 99,
* MATOMBIG = 99,
* MION = 90,
* MION0 = 9,
* MMOLEC=500,
* MPHOT = 10,
* MZZ = 2,
* MMER = 2,
* NLMX = 80,
* MI1 = MION0-1,
* MLINH = 78,
* MHT = 7,
* MHE = 20,
* MHWL = 55)
PARAMETER (MFGRID = 100000,
* MTTAB = 21,
* MRTAB = 20,
* MSFTAB = 6000000)
parameter (mfhtab=1000,
* mtabth=10,
* mtabeh=10)
c
C Basic physical constants
C
PARAMETER (H = 6.6256D-27,
* CL = 2.997925D10,
* BOLK = 1.38054D-16,
* HK = 4.79928144D-11,
* EH = 2.17853041D-11,
* BN = 1.4743D-2,
* SIGE = 6.6516D-25,
* PI4H = 1.8966D27,
* HMASS = 1.67333D-24)
C
C Unit number
C
PARAMETER (IBUFF=95)
C
C Variables to hold quantum numbers limits
C (see LEVLIMITS below)
C
INTEGER*4 SQUANT1(MLEVEL),SQUANT2(MLEVEL),
* LQUANT1(MLEVEL),LQUANT2(MLEVEL),
* PQUANT1(MLEVEL),PQUANT2(MLEVEL)
C
C Basic parameters
C
COMMON/BASNUM/NATOM,
* NION,
* NLEVEL,
* ND,NDSTEP,
* NFREQ,NFROBS,NFREQC,NFREQS,
* NMU
COMMON/LTESET/LTE,LTEGR
COMMON/INPPAR/TEFF,
* GRAV,
* YTOT(MDEPTH),
* WMM(MDEPTH),
* WMY(MDEPTH),
* vaclim,
* ATTOT(MATOM,MDEPTH)
COMMON/BASICM/IMODE,
* IMODE0,
* IFREQ,
* INLTE,
* IDSTD,
* IFWIN,
* IFEOS,
* IBFAC
COMMON/INTKEY/INMOD,INTRPL,ICHANG,ICHEMC,IATREF,ICONTL
COMMON/LBLANK/IBLANK,NBLANK
COMMON/NXTINI/ALM00,ALST00,NXTSET,INLIST,ALAMBE,DLAMLO
COMMON/IPRNTR/IPRIN
C
C Parameters for explicit atoms
C
COMMON/ATOPAR/AMASS(MATEX),
* ABUND(MATEX,MDEPTH),
* RELAB(MATEX,MDEPTH),
* NUMAT(MATEX),
* N0A(MATEX),
* NKA(MATEX),
* SABND(MATEX)
C
C Parameters for explicit ions
C
COMMON/IONPAR/FF(MIOEX),
* NFIRST(MIOEX),
* NLAST(MIOEX),
* NNEXT(MIOEX),
* IUPSUM(MIOEX),
* IZ(MIOEX),
* IFREE(MIOEX),
* INBFCS(MIOEX),
* ILIMITS(MIOEX)
C
C Parameters for explicit levels
C
COMMON/LEVPAR/ENION(MLEVEL),
* G(MLEVEL),
* NQUANT(MLEVEL),
* IATM(MLEVEL),
* IEL(MLEVEL),
* ILK(MLEVEL),
* ifwop(mlevel),
* isemex(matom)
C
C Limits for explicit levels
C
COMMON/LEVLIMITS/ENION1(MLEVEL),
* ENION2(MLEVEL),
* SQUANT1,
* SQUANT2,
* LQUANT1,
* LQUANT2,
* PQUANT1,
* PQUANT2
C
C Parameters for all considered transitions
C
COMMON/TRAPAR/IBF(MLEVEL),
* S0BF(MLEVEL),
* ALFBF(MLEVEL),
* BETBF(MLEVEL),
* GAMBF(MLEVEL)
C
COMMON/MRGPAR/SGM0(MMER),
* FRCH(MMER),
* SGEXT1(MMER,MDEPTH),
* GMER(MMER,MDEPTH),
* SGMSUM(NLMX,MMER,MDEPTH),
* SGMG(MMER,MDEPTH),
* IMRG(MLEVEL),
* IIMER(MMER)
C
COMMON/DWNPAR/ELEC23(MDEPTH),
* Z3(MZZ),
* DWC1(MZZ,MDEPTH),
* DWC2(MDEPTH)
C
C additional opacities
c
COMMON/OPCPAR/IOPADD,
* IOPHMI,
* IOPH2P,
* IOPHEM,
* IOPCH,
* IOPOH,
* IOPH2M,
* IOH2H2,IOH2HE,IOH2H1,IOHHE,
* IOPHLI,
* IRSCT,
* IRSCHE,
* IRSCH2
C
C Auxiliary parameters
C
COMMON/AUXIND/IATH,IELH,IELHM,N0H,N1H,NKH,N0HN,N0M,
* IATHE,IELHE1,IELHE2
COMMON/MOLFLG/TMOLIM,MOLIND(11000),NMOLEC,IFMOL,
* MOLTAB,IRWTAB,IIRWIN,IPFEXO
COMMON/QFLAGS/ERANGE,ISPICK,ILPICK,IPPICK
C
C Parameters for atoms considered in line blanketing opacity
C
LOGICAL LGR(MATOM),LRM(MATOM)
COMMON/PFSTDS/PFSTD(MION,MATOM),MODPF(MATOM)
COMMON/ADDPOP/RR(MATOM,MION)
COMMON/ATOBLN/ENEV(MATOM,MI1),AMAS(MATOM),ABND(MATOM),
* ABNDD(MATOM,MDEPTH),ABNREF(MDEPTH),TYPAT(MATOM),
* IATEX(MATOM),INPOT(MATOM,MION0)
COMMON/ATOINI/NATOMS,IONIZ(MATOM),LGR,LRM
c
c parameters for hydrogen Stark broadening tables
c
COMMON/HYDPRF/PRFHYD(MLINH,MDEPTH,MHWL),
* WLHYD(MLINH,MHWL),
* NWLHYD(MLINH),
* WL(MHWL,MLINH),
* XT(MHT,MLINH),
* XNE(MHE,MLINH),
* PRF(MHWL,MHT,MHE,MLINH),
* WLINE(4,22),
* NWLH(MLINH),
* NTH(MLINH),
* NEH(MLINH),
* ILIN0(4,22),
* ILEMKE,
* NLIHYD
COMMON/AUXHYD/XK,FXK,BETAD,DBETA,BERGFC,CUTLYM,CUTBAL
COMMON/HHEPRF/IHYDPR,IHE1PR,IHE2PR
COMMON/HYLPAR/IHYL,ILOWH,M10,M20
COMMON/HYLPAW/IHYLW(MFREQ),ILOWHW(MFREQ),
* M10W(MFREQ),M20W(MFREQ)
COMMON/HE2PAR/IFHE2,IHE2L,ILWHE2,MHE10,MHE20
COMMON/HE2PAW/IHE2LW(MFREQ),ILWHEW(MFREQ),
* MHE10W(MFREQ),MHE20W(MFREQ)
C
C parameters for the macroscopic velocity field and angles
C
COMMON/VELPAR/ANGL(MMU),WANGL(MMU),VELC(MDEPTH),NMU0,IFLUX
+10
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COMMON/FREQSY/FREQ(MFREQ),W(MFREQ),WLAM(MFREQ),
* FRX1(MFREQ),FRX2(MFREQ),BNUE(MFREQ),
* FRQOBS(MFREQ),WLOBS(MFREQ),
* FREQC(MFREQC),WLAMC(MFREQC),
* IJCINT(MFREQ)
COMMON/CRSAVG/FRECR(MCROSS,MFCRA),CROSR(MCROSS,MFCRA),
* CRMX(MCROSS),NFCR(MCROSS),IASV
COMMON/CRSAVQ/FRECQ(MPHOT,MFCRA),QHOT(MPHOT,MFCRA),
* AQHT(MPHOT),EQHT(MPHOT),GQHT(MPHOT),
* CRMY(MPHOT),NFQHT(MPHOT),NQHT
+15
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PARAMETER (MRCORE=20,
* MKU=MDEPTH+MRCORE,
* MEXT=MKU)
COMMON/COMANG/BMU(MKU,MDEPTH),WMUJ(MKU,MDEPTH),WMUH(MKU)
COMMON/CORADI/RD(MDEPTH),RCORE,RFNORM,PIM(MKU),RAD1(MDEPTH),
* DELZ(MKU,MDEPTH),NUD(MKU),NUDF(MKU),KMU,NREXT,
* NRCORE,NFIRY,NDF
COMMON/CORAF/DELZF(MEXT,MDEPF ),DFRQF(MEXT,2*MDEPF )
COMMON/COVEL/VEL(MDEPTH),DFRQ(MKU,2*MDEPTH),DVD(MDEPTH),
* XMDOT,XMD4,BETAV,VINF
COMMON/EXTMOD/FFQ(MOPAC),FFQV(MOPAC),RDF(MDEPF ),DENSF(MDEPF ),
* VELF(MEXT,MDEPF ),DRAY(MEXT,2*MDEPF ),
* KRAY(MEXT,2*MDEPF ),NOPAC
COMMON/OPAVEL/WDIL(MDEPTH),PLANW(MDEPTH),TRAD(MTRAD,MDEPTH),
* DENSCON(MDEPTH)
Binary file not shown.
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program list2bin
c ================
c
c transforms an ASCII line list to a binary
c
c INPUT: std input - ASCII list
c
c OUTPUT: fort.12 - binary list
c std. output gives an info on number of lines
c
implicit real*8 (a-h,o-z)
character*102 rec
dimension x(10),j(7)
c
c first, find the format of the line list by examining the 1st record
c
n=1
npr=10
npi=7
read(5,'(a102)') rec
write(*,*) rec
read(rec,*,iostat=kst) (x(i),i=1,10),(j(i),i=1,7)
if(kst.ne.0) then
read(rec,*,iostat=kst1) (x(i),i=1,10),j(1)
npr=10
npi=1
if(kst1.ne.0) then
read(rec,*,iostat=kst2) (x(i),i=1,9)
npr=9
npi=0
if(kst2.ne.0) then
read(rec,*,iostat=kst3) (x(i),i=1,7)
npr=7
npi=0
if(kst3.ne.0) then
read(rec,*,iostat=kst4) (x(i),i=1,4)
npr=4
npi=0
if(kst4.ne.0) then
write(*,*)
* 'no applicable format of the line list detected'
stop
end if
end if
end if
end if
end if
c
write(6,600) npr,npi
600 format('number of parameters in the list; real,int:',2i4)
write(12) (x(i),i=1,npr),(j(i),i=1,npi)
c
c read the list and transport to binary
c
10 continue
read(5,*,err=10,end=20) (x(i),i=1,npr),(j(i),i=1,npi)
n=n+1
write(12) (x(i),i=1,npr),(j(i),i=1,npi)
go to 10
20 continue
c
write(6,601) n
601 format(i10,' lines included in the binary file fort.12')
end
+53
View File
@@ -0,0 +1,53 @@
#
# makefile for synspec/rotin
# Carlos 2019
#
F90 = gfortran
OPT= -fno-automatic
#F90 = g95
#OPT= -fstatic -Wl,--no-relax
#F90 = sunf95
#OPT = -Bstatic -xmodel=medium
#F90 = ifort
#OPT = -shared-intel -mcmodel medium
#F90 = nvfortran
#OPT = -Bstatic -mcmodel=medium
UNAME_S := $(shell uname -s)
ifeq ($(UNAME_S),Linux)
OPT += -mcmodel=medium
endif
all: compile install
compile: synspec54 rotin list2bin
synspec54: synspec54.f LINDAT.FOR MODELP.FOR PARAMS.FOR SYNTHP.FOR WINCOM.FOR
${F90} ${OPT} synspec54.f -o synspec54
rotin: rotin.f
${F90} ${OPT} rotin.f -o rotin
list2bin: list2bin.f
${F90} ${OPT} list2bin.f -o list2bin
install: ../bin ../bin/synspec54 ../bin/rotin ../bin/list2bin
../bin/synspec54 ../bin/rotin ../bin/list2bin: synspec54 rotin list2bin
cp synspec54 ../bin/
cp rotin ../bin/
cp list2bin ../bin/
../bin:
mkdir ../bin
clean:
rm -f synspec54 rotin list2bin ../bin/synspec54 ../bin/rotin ../bin/list2bin
+288
View File
@@ -0,0 +1,288 @@
program ngrid
C =============
c
IMPLICIT REAL*8 (A-H, O-Z)
PARAMETER (MFGRID = 300000,
* MTTAB = 25,
* MRTAB = 15,
* MSFTAB = 6000000)
c
real*4 absgrd(mttab,mrtab,mfgrid)
common/gridp0/tempg(mttab),densg(mrtab),elecgr(mttab,mrtab),
* densg0(mttab),temp1,ntemp,ndens
common/gridf0/wlgrid(mfgrid),nfgrid
common/fintab/absgrd
common/initab/absop(msftab),wltab(msftab)
common/elecm0/elecm(mttab)
dimension tempvec(mttab),rhovec(mrtab)
dimension abgrd(mfgrid),abunt(30),abuno(30)
dimension typa(30)
character*(80) tabname,optable
character*4 typa
c
istop=0
read(5,*) nlamb,inttab,wlam1,wlam2
read(5,*) tabname,ibingr
if(nlamb.gt.mfgrid) then
write(*,*) 'nlambda.gt.mfgrid - recompile with larger mfgrid'
istop=1
end if
ibinop=0
read(5,*,err=5,end=5) optable,ibinop
5 continue
write(*,*) 'original optable ',optable
c
nfgrid=nlamb
wl1=log(wlam1)
wl2=log(wlam2)
dwl=(wl2-wl1)/(nfgrid-1)
do i=1,nfgrid
wlgrid(i)=exp(wl1+(i-1)*dwl)
end do
c
c read the header of the old opacity table
c
if(ibinop.eq.0) then
open(52,file=optable,status='old')
else
open(52,file=optable,form='unformatted',status='old')
end if
c
if(ibinop.eq.0) then
read(52,*)
read(52,*)
do iat=1,30
read(52,*) typa(iat),abunt(iat),abuno(iat)
end do
read(52,*)
read(52,*)
read(52,*) ifmolt,tmolit
read(52,*)
read(52,*)
read(52,*) iophmt,ioph2t,iophet,iopcht,iopoht
read(52,*)
read(52,*)
read(52,*) numfre0,numtem0,numrh0
read(52,*)
read(52,*) (tempvec(i),i=1,numtem0)
read(52,*)
read(52,*) (rhovec(j),j=1,numrh0)
read(52,*)
read(52,*) ((elecgr(i,j),j=1,numrh0),i=1,numtem0)
else
do iat=1,30
read(52) typa(iat),abunt(iat),abuno(iat)
end do
read(52) ifmolt,tmolit
read(52) iophmt,ioph2t,iophet,iopcht,iopoht
read(52) numfre0,numtem0,numrh0
read(52) (tempvec(i),i=1,numtem0)
read(52) (rhovec(j),j=1,numrh0)
read(52) ((elecgr(i,j),j=1,numrh0),i=1,numtem0)
end if
ntemp=numtem0
ndens=numrh0
write(*,*) 'ntemp,ndens',ntemp,ndens
if(ntemp.gt.mttab) then
write(*,*) 'ntemp.gt.mttab - recompile with larger mttab'
istop=1
end if
if(ndens.gt.mrtab) then
write(*,*) 'ndens.gt.mrtab - recompile with larger mrtab'
istop=1
end if
c
if(istop.eq.1) stop
c
c read file fort.27 (internal opacitis) and set the
c arrays for the new opacity tables
c
if(inttab.ne.1) then
c
c 1st possibility - approximate preserving an integral of opacity
c
indext=0
indexn=0
nfr=0
10 continue
indext=indext+1
20 continue
indexn=indexn+1
nfr=0
ijgrd=0
30 continue
ijgrd=ijgrd+1
wlgr=0.5*(wlgrid(ijgrd)+wlgrid(ijgrd+1))
isum=0
sum=0.
40 continue
read(27,*,err=50,end=50) ip,wl,abl
if(wl.le.wlgr) then
sum=sum+exp(abl)
isum=isum+1
if(ip.le.nfr) go to 50
nfr=ip
go to 40
end if
abgrd(ijgrd)=log(sum/float(isum))
if(ijgrd.lt.nfgrid) go to 30
50 continue
write(*,*) 'it,ir,nf',indext,indexn,nfr,nfgrid
do ij=1,nfgrid
absgrd(indext,indexn,ij)=real(abgrd(ij))
end do
absgrd(indext,indexn,nfgrid)=absgrd(indext,indexn,nfgrid-1)
c
if(indexn.lt.ndens) then
go to 20
else
indexn=0
end if
if(indext.lt.ntemp) then
go to 10
else
indext=0
end if
c
else
c
c 2nd possibility - an interpolation in wavelengths
c
indext=0
indexn=0
nfr=0
110 continue
indext=indext+1
120 continue
indexn=indexn+1
nfr=0
130 continue
read(27,*,err=150,end=150) ip,wl,abl
if(ip.le.nfr) go to 150
wltab(ip)=wl
absop(ip)=abl
nfr=ip
go to 130
150 continue
write(*,*) 'it,ir,nf',indext,indexn,nfr,nfgrid
call intrp(wltab,absop,wlgrid,abgrd,nfr,nfgrid)
do ij=1,nfgrid
absgrd(indext,indexn,ij)=real(abgrd(ij))
end do
c
if(indexn.lt.ndens) then
go to 120
else
indexn=0
end if
if(indext.lt.ntemp) then
go to 110
else
indext=0
end if
end if
c
c store the opacities in the new table
c
if(ibingr.eq.0) then
open(53,file=tabname,status='unknown')
write(53,600)
do iat=1,30
write(53,601) typa(iat),abunt(iat),abuno(iat)
end do
write(53,602) ifmolt,tmolit
write(53,603) iophmt,ioph2t,iophet,iopcht,iopoht
write(53,611) nfgrid,ntemp,ndens
write(53,612) (tempvec(i),i=1,ntemp)
write(53,613) (rhovec(j),j=1,ndens)
write(53,614) ((elecgr(i,j),j=1,ndens),i=1,ntemp)
do k = 1, nfgrid
write(53,615) k,wlgrid(k),2.997925e18/wlgrid(k)
do j = 1,ndens
write(53,616) (absgrd(i,j,k),i=1,ntemp)
end do
end do
600 format('opacity table with element abundances:'/
* 'element for EOS for opacities')
601 format(' ',a4,1p2e12.3)
602 format(/'molecules - ifmol,tmolim:'/,i4,f10.1)
603 format('additional opacities'/' H- H2+ He- CH OH'/
* 5i4)
611 format(/'number of frequencies, temperatures, densities:'
* /10x,3i10)
612 format('log temperatures'/(6F11.6))
613 format('log densities'/(6F11.6))
614 format('log electron densities from EOS'/(6f11.6))
615 format(/' *** frequency # : ',i8,f15.5/1pe20.8)
616 format((1p6e14.6))
else
do iat=1,30
write(63) typa(iat),abunt(iat),abuno(iat)
end do
write(63) ifmolt,tmolit
write(63) iophmt,ioph2t,iophet,iopcht,iopoht
write(63) nfgrid,ntemp,ndens
write(63) (tempvec(i),i=1,ntemp)
write(63) (rhovec(j),j=1,ndens)
write(63) ((elecgr(i,j),j=1,ndens),i=1,ntemp)
do k = 1, nfgrid
write(63) wlgrid(k)
do j = 1, ndens
write(63) (absgrd(i,j,k),i=1,ntemp)
end do
end do
end if
c
end
C
C
C ****************************************************************
C
C
subroutine intrp(wltab,absop,wlgrid,abgrd,nfr,nfgrid)
c =====================================================
c
IMPLICIT REAL*8 (A-H, O-Z)
PARAMETER (MFGRID = 400000)
c
dimension wltab(1),absop(1),wlgrid(1),abgrd(1)
dimension yint(mfgrid),jint(mfgrid)
c
c set up interpolation coefficients for frequency interpolation
c by bisection
c
fr1=wltab(1)
fr2=wltab(nfr)
do ij=1,nfgrid
xint=wlgrid(ij)
jl=0
ju=nfr+1
10 continue
if(ju-jl.gt.1) then
jm=(ju+jl)/2
if((fr2.gt.fr1).eqv.(xint.gt.wltab(jm))) then
jl=jm
else
ju=jm
end if
go to 10
end if
j=jl
if(j.eq.nfr) j=j-1
if(j.eq.0) j=j+1
jint(ij)=j
c yint(ij)=un/log10(wltab(j+1)/wltab(j))
yint(ij)=1./(wltab(j+1)-wltab(j))
end do
c
do ij=1,nfgrid
j=jint(ij)
rc=(absop(j+1)-absop(j))*yint(ij)
c abgrd(ij)=rc*log10(wlgrid(ij)/wltab(j))+absop(j)
abgrd(ij)=rc*(wlgrid(ij)-wltab(j))+absop(j)
end do
c
return
end
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