distribution_source_identifierΒΆ
Translation table for Heating and Current Drive (HCD) distsource types, i.e. types particles source in Fokker-Planck equation (from NBI and nuclear reactions).
Name |
Index |
Description |
Units |
Alias |
|---|---|---|---|---|
unspecified |
0 |
unspecified |
None |
None |
NBI |
1 |
Source from neutral beam injection |
None |
None |
nuclear |
100 |
Source from nuclear reaction (reaction type unspecified) |
None |
None |
H_H_to_D_positron_nu |
101 |
Source from nuclear reaction: H+H->D+positron+neutrino |
None |
None |
H_D_to_3He_gamma |
102 |
Source from nuclear reaction: H+D->3He+gamma |
None |
H_D_to_He3_gamma |
H_T_to_3He_n |
103 |
Source from nuclear reaction: H+T->3He+neutron |
None |
H_T_to_He3_n |
H_3He_to_4He_positron_nu |
104 |
Source from nuclear reaction: H+3He->4He+positron+neutrino |
None |
H_He3_to_He4_positron_nu |
D_D_to_T_H |
105 |
Source from nuclear reaction: D+D->T+H |
None |
None |
D_D_to_3He_n |
106 |
Source from nuclear reaction: D+D->3He+neutron |
None |
D_D_to_He3_n |
D_T_to_4He_n |
107 |
Source from nuclear reaction: T+D->4He+neutron |
None |
D_T_to_He4_n |
D_3He_to_4He_H |
108 |
Source from nuclear reaction: 3He+D->4He+H |
None |
D_He3_to_He4_H |
T_T_to_4He_n_n |
109 |
Source from nuclear reaction: T+T->4He+neutron+neutron |
None |
T_T_to_He4_n_n |
T_3He_to_4He_H_n |
110 |
Source from nuclear reaction: 3He+T->4He+H+neutron |
None |
T_He3_to_He4_H_n |
3He_3He_to_4He_H_H |
111 |
Source from nuclear reaction: 3He+3He->4He+neutron+neutron |
None |
He3_He3_to_He4_H_H |
3He_4He_to_7Be_gamma |
112 |
Source from nuclear reaction: 3He+4He->7Be+gamma |
None |
He3_He4_to_Be7_gamma |
6Li_n_to_4He_T |
113 |
Source from nuclear reaction: 6Li+n->4He+T |
None |
Li6_n_to_He4_T |
7Li_n_to_4He_T_n |
114 |
Source from nuclear reaction: 7Li+n->4He+T+n |
None |
Li7_n_to_He4_T_n |
runaway |
1000 |
Source from runaway processes |
None |
None |