function cion(n,j,e,t) c c collisional ionization rate from Raymond c rate is returned in units cm^3/s c inputs are: n=nuclear charge, c j=ion stage c e=valence shell ionization threshold (in eV) c t=temperature in K. c c Tim Kallman's routine for calculating collisional ionization rates. c Note that this routine only accounts for valence shell ionization. c It should be called only once for each ion stage and the valence c shell ionization threshold should be the lowest one (e.g. the 2p c ionization potential for CI). c c INCLUDE 'IMPLIC.FOR' c c sm younger jqsrt 26, 329; 27, 541; 29, 61 with moores for undone c a0 for b-like ion has twice 2s plus one 2p as in summers et al c chi = kt / i c dimension a0(30),a1(30),a2(30),a3(30),b0(30),b1(30), & b2(30),b3(30),c0(30),c1(30),c2(30),c3(30), & d0(30),d1(30),d2(30),d3(30) c data a0/13.5,27.0,9.07,11.80,20.2,28.6,37.0,45.4, & 53.8,62.2,11.7,38.8,37.27,46.7,57.4,67.0, & 77.8,90.1,106.,120.8,135.6,150.4,165.2,180.0, & 194.8,209.6,224.4,239.2,154.0,268.8/ data a1/ - 14.2,-60.1,4.30,27*0./ data a2/40.6,140.,7.69,27*0./ data a3/ - 17.1,-89.8,-7.53,27*0./ c data b0/ - 4.81,-9.62,-2.47,-3.28,-5.96,-8.64,-11.32, & -14.00,-16.68,-19.36,-4.29,-16.7,-14.58,-16.95, & -19.93,-23.05,-26.00,-29.45,-34.25,-38.92, & -43.59,-48.26,-52.93,-57.60,-62.27,-66.94, & -71.62,-76.29,-80.96,-85.63/ data b1/9.77,33.1,-3.78,27*0./ data b2/ - 28.3,-82.5,-3.59,27*0./ data b3/11.4,54.6,3.34,27*0./ c data c0/1.85,3.69,1.34,1.64,2.31,2.984,3.656,4.328, & 5.00,5.672,1.061,1.87,3.26,5.07,6.67,8.10, & 9.92,11.79,7.953,8.408,8.863,9.318,9.773, & 10.228,10.683,11.138,11.593,12.048,12.505,12.96/ data c1/0.,4.32,.343,27*0./ data c2/0.,-2.527,-2.46,27*0./ data c3/0.,.262,1.38,27*0./ c data d0/ - 10.9,-21.7,-5.37,-7.58,-12.66,-17.74, & -22.82,-27.9,-32.98,-38.06,-7.34,-28.8,-24.87, & -30.5,-37.9,-45.3,-53.8,-64.6,-54.54,-61.70, & -68.86,-76.02,-83.18,-90.34,-97.50,-104.66, & -111.82,-118.98,-126.14,-133.32/ data d1/8.90,42.5,-12.4,27*0./ data d2/ - 35.7,-131.,-8.09,27*0./ data d3/16.5,87.4,1.23,27*0./ c cion = 0. chir = t/(11590.*e) if ( chir.le..0115 ) return chi=chir if(chi.lt.0.1) ch=0.1 ch2 = chi*chi ch3 = ch2*chi alpha = (.001193+.9764*chi+.6604*ch2+.02590*ch3) & /(1.0+1.488*chi+.2972*ch2+.004925*ch3) beta = (-.0005725+.01345*chi+.8691*ch2+.03404*ch3) & /(1.0+2.197*chi+.2457*ch2+.002503*ch3) j2 = j*j j3 = j2*j iso = n - j + 1 c a = a0(iso) + a1(iso)/j + a2(iso)/j2 + a3(iso)/j3 b = b0(iso) + b1(iso)/j + b2(iso)/j2 + b3(iso)/j3 c = c0(iso) + c1(iso)/j + c2(iso)/j2 + c3(iso)/j3 d = d0(iso) + d1(iso)/j + d2(iso)/j2 + d3(iso)/j3 c c fe ii experimental ionization montague et al: d. neufeld fit if ( n.eq.26 .and. j.eq.2 ) then a = -13.825 b = -11.0395 c = 21.07262 d = 0. endif c ch = 1./chi fchi = 0.3*ch*(a+b*(1.+ch)+(c-(a+b*(2.+ch))*ch)*alpha+d*beta*ch) cion = 2.2e-6*sqrt(chir)*fchi*expo(-1./chir)/(e*sqrt(e)) return end