List of the 12th most important reactions in the BBN network
|
code index |
reaction |
adopted |
options |
1 |
12 |
|
ando |
ando skm |
2 |
16 |
|
stlb |
stlb de04 skm |
3 |
17 |
|
ntof |
ntof cy04 skm |
4 |
19 |
|
ntof |
wag ntof |
5 |
20 |
|
il16 |
il16 skm |
6 |
24 |
|
stlb |
stlb cf88 de04 skm |
7 |
26 |
|
stlb |
stlb skm |
8 |
27 |
|
il16 |
il16 ncr2 skm cd08 |
9 |
28 |
|
stlb |
stlb skm |
10 |
29 |
|
stlb |
stlb skm |
11 |
30 |
|
stlb |
stlb de04 cf88 skm |
12 |
31 |
|
stlb |
stlb de04 skm |
#wag : Wagoner, R.V., ApJS, 18, 247 (1969)
#cf88 : Caughlan and Fowler, ADNDT 40, 283 (1988)
#skm : Smith, Kawano and Malaney, ApjS 85, 2019 (1993)
#de04 : Descouvemont et al. ADNDT 88, 203 (2004)
#cy04 : Cyburt, PRD 70, 023505 (2004)
#ando : Ando et al. Phys. Rev. C 74, 025809 (2006)
#il16 : Iliadis et al., ApJ 831, 107 (2016)
#ncr2 : fit to ncare2 library
#stlb : fit to starlib table
#ntof : rate from n_TOF experiments
Code segments of the individual reaction rates adopted in the present BBN calculations
1/* H + n -> g + H2 */
2/* rate from Ando et al. Phys. Rev. C 74, 025809 (2006) */
3/* p + n -> d + g */
4 a0 = 44216.0; a1 = 3.75191; a2 = 1.92934; a3 = 0.746503; a4 = 0.0197023; a5 = 3.00491e-6;
5 b1 = 5.4678; b2 = 5.62395; b3 = 0.489312; b4 = 0.00747806;
6 f[12]=a0*(1. + a1*T9 + a2*pow(T9,2.) + a3*pow(T9,3.) + a4*pow(T9,4.) + a5*pow(T9,5.))/(1. + b1*T9 + b2*pow(T9,2.) + b3*pow(T9,3.) + b4*pow(T9,4.));
1* He3 + n -> p + H3 */
2/* starlib rate parameters - de04 data */
3 a0 = 6.89423e+08; a1 = -0.4347; a2 = -0.199323; a3 = 0.590373; a4 = -0.322449; a5 = 0.0742735; a6 = -0.00648816;
4 f[16] = a0*(1. + a1*pow(T9,1./2.) + a2*T9 + a3*pow(T9,3./2.) + a4*pow(T9,2.) + a5*pow(T9,5./2.) + a6*pow(T9,3.));
1* Be7 + n -> p + Li7 */
2/* rate from n_TOF - central value */
3 a0= 6.8048e+09; a1= -1.9706e+00; a2= 2.0419e+00; a3= -1.0687e+00; a4= 2.7172e-01; a5= -2.6699e-02; a6= 1.9610e+08; a7= 2.8899e+07; b0= 2.8114e-01;
4 f[17] = a0*(1. + a1*pow(T9,1./2.) + a2*T9 + a3*pow(T9,3./2.) + a4*T9*T9 + a5*pow(T9,5./2.)) + a6*pow(T9/(1.+13.076*T9),3./2.)/pow(T9,3./2.) + a7/pow(T9,3./2.)*exp(-b0/T9);
5
6/* rate from n_TOF - upper */
7 a0= 6.8181e+09; a1= -1.6226e+00; a2= 1.4457e+00; a3= -6.7629e-01; a4= 1.5737e-01; a5= -1.4373e-02; a6= 7.3135e+08; a7= -2.8413e+08; b0= 8.1347e-01;
8 f[17] = a0*(1. + a1*pow(T9,1./2.) + a2*T9 + a3*pow(T9,3./2.) + a4*T9*T9 + a5*pow(T9,5./2.)) + a6*pow(T9/(1.+13.076*T9),3./2.)/pow(T9,3./2.) + a7/pow(T9,3./2.)*exp(-b0/T9);
9
10/* rate from n_TOF - lower */
11 a0= 7.5185e+09; a1= -2.4307e+00; a2= 2.9935e+00; a3= -1.7338e+00; a4= 4.6746e-01; a5= -4.7572e-02; a6= -9.7708e+08; a7= -7.0378e+09; b0= 3.1868e+00;
12 f[17] = a0*(1. + a1*pow(T9,1./2.) + a2*T9 + a3*pow(T9,3./2.) + a4*T9*T9 + a5*pow(T9,5./2.)) + a6*pow(T9/(1.+13.076*T9),3./2.)/pow(T9,3./2.) + a7/pow(T9,3./2.)*exp(-b0/T9);
1/* Be7 + n -> a + He4 */
2/* n_TOF rate as in Barbagallo et al. PRL 117 (2016) 152701 */
3 f[19]=4.81e+5 + 1.84e+6*T9 + 3.03e+6*pow(T9,1.5);
1/* H2 + p -> g + He3 */
2/* rate from Iliadis et al. (2016) fit */
3 a0= 2.452e+03; b0= 3.732e+00; a1= -1.632e+00; a2= 7.609e+00; a3= -6.133e+00; a4= 6.557e+00; a5= -1.042e+00;
4 f[20]=a0*pow(T9,-2./3.)*exp(-b0*pow(T9,-1./3.))*(1. + a1*pow(T9,1./3.) + a2*pow(T9,2./3.) + a3*T9 + a4*pow(T9,4./3.) + a5*pow(T9,5./3.));
1/* Li7 + p -> a + He4 */
2/* starlib rate parameters - de04 data */
3 a0 = 1.45251e+09; b0 = 8.44454; a1 = -6.76368e+08; b1 = 8.41908; a2 = 4.0217e+09; b2 = 25.3862; b3 = 0.16592;
4 f[24] = a0/pow(T9,2./3.)*exp(-b0/pow(T9,1./3.)) + a1*pow(T9/(1.0+b3*T9),5./6.)/pow(T9,3./2.)*exp(-b1/pow(T9/(1.0+b3*T9),1./3.))+a2/pow(T9,3./2.)*exp(-b2/T9);
1/* H3 + a -> g + Li7 original */
2/* starlib rate parameters - in17 data */
3 a0= 1.3350e+05; b0= 8.0768e+00; a1= 5.9164e+00; a2= -1.3045e+01; a3= 1.3315e+01; a4= -6.4673e+00; a5= 1.3420e+00; a6= 5.1090e+05; b1= 8.0680e+00;
4 f[26]=a0/pow(T9,2./3.)*exp(-b0/pow(T9,1./3.))*(1.+a1*pow(T9,1./3.)+a2*pow(T9,2./3.) + a3*T9 + a4*pow(T9,4./3.) + a5*pow(T9,5./3.)) + a6*pow(T9/(1.+0.1378*T9),5./6.)/pow(T9,3./2.)*exp(-b1/pow(T9/(1.+0.1378*T9),1./3.));
1/* He3 + a -> g + Be7 */
2/* rate from Iliadis et al. (2016) fit */
3 a0= 9.8079e+06; b0= 1.4192e+01; a1= -1.3272e+00; a2= 1.9911e-01; a3= 1.0387e+00; a4= -6.7320e-01; a5= 1.2511e-01; a6= 6.1164e+06; b1= 1.2829e+01;
4 T9F=T9/(1.+0.1071*T9);
5 f[27]= a0*pow(T9,-2./3.)*exp(-b0/pow(T9,1./3.))*(1.+a1*pow(T9,1./3.) + a2*pow(T9,2./3.) + a3*T9 + a4*pow(T9,4./3.) + a5*pow(T9,5./3.)) + a6*pow(T9F,5./6.)*pow(T9,-3./2.)*exp(-b1/pow(T9F,1./3.));
1/* H2 + H2 -> n + He3 */
2/* starlib rate parameters - in17 data */
3 a0 = 3.95e+8; b0 = 4.259; a1 = 0.098; a2 = 1.00239; a3 = 1.08419; a4 =-0.743092; a5 = 0.139404;
4 f[28]=a0*pow(T9,-2./3.)*exp(-b0/pow(T9,1./3.))*(1.+a1*pow(T9,1./3.)+a2*pow(T9,2./3.)+a3*T9+a4*pow(T9,4./3.)+a5*pow(T9,5./3.));
1/* H2 + H2 -> p + H3 */
2/* starlib rate parameters - in17 data */
3 a0 = 4.12649e+08; b0 = 4.258; a1 = 0.304711; a2 = -0.446767; a3 = 2.23021; a4 = -1.19482; a5 = 0.210592;
4 f[29]= a0*pow(T9,-2./3.)*exp(-b0/pow(T9,1./3.))*(1.+a1*pow(T9,1./3.)+a2*pow(T9,2./3.)+a3*T9+a4*pow(T9,4./3.)+a5*pow(T9,5./3.));
1/* H3 + H2 -> n + He4 */
2/* starlib rate parameters - de04 data */
3 a0 = 6.32853e+10; b0 = 4.52388; b1 = 0.072028; a1 = 6.47865; a2 = -29.3575; a3 = 4.35456; a4 = 280.001; a5 = -253.094; a6 = 7.56418e+08; b2 = 0.472317;
4 f[30]=a0*pow(T9,-2./3.)*exp(-b0/pow(T9,1./3.)-pow(T9/b1,2.))*(1. + a1*pow(T9,1./3.) + a2*pow(T9,2./3.) + a3*T9 + a4*pow(T9,4./3.) + a5*pow(T9,5./3.)) + a6*pow(T9,-2./3.)*exp(-b2/T9);
1/* He3 + H2 -> p + He4 */
2/* starlib rate parameters - de04 data */
3 a0 = 2.46165e+10; b0 = 7.15127; b1 = 0.241809; a1 = 8.69492; a2 = -22.7967; a3 = 21.7527; a4 = 6.97; a5 = 34.9149; a6 = 4.82217e+08; b2 = 1.71366;
4 f[31]=a0*pow(T9,-2./3.)*exp(-b0/pow(T9,1./3.)-pow(T9/b1,2.))*(1.+ a1*pow(T9,1./3.)+ a2*pow(T9,2./3.) + a3*T9 + a4*pow(T9,4./3.) + a5*pow(T9,5./3.)) + a6/pow(T9,1./2.)*exp(-b2/T9);
--
AlbertoMengoni - 2018-02-20