Note: If this is not the first time Netgen is run from your current
IP address, it might be necessary to click first on `Clear network'; otherwise,
the selected reactions will be appended to the network generated by the
previous Netgen run.
Then click on button 'Generate network' and
proceed to step 1b below.
Here is a screen copy of the form corresponding to step 1a.
It is not yet possible to edit the network at this stage, e.g. by removing some reactions. This will be possible in a future release of Netgen.
Results are described in step 1c.
Here is a screen copy of the form corresponding to step 1b.
bib_code Reaction 1 1 C 11 ( 1 PROT , 0 OOOOO) 1 N 12 1 1 C 11 ( 1 PROT , 1 HE 4) 1 B 8 1 1 C 11 ( 0 OOOOO, 0 OOOOO) 1 B 11 1 1 C 12 ( 1 PROT , 0 OOOOO) 1 N 13 1 1 C 12 ( 1 PROT , 1 NEUT ) 1 N 12 1 1 C 12 ( 1 PROT , 1 HE 4) 1 B 9 1 1 C 13 ( 1 PROT , 0 OOOOO) 1 N 14 .........................
1 1 F 20 ( 1 PROT , 0 OOOOO) 1 NE 21 1 1 F 20 ( 1 PROT , 1 NEUT ) 1 NE 20 1 1 F 20 ( 1 PROT , 1 HE 4) 1 O 17 1 1 F 20 ( 0 OOOOO, 0 OOOOO) 1 NE 20
What is to be found in the table of reaction rates?
This table provides the number of reactions per sec per (cm3mole-1)(N-1), where N refers to the number of particles in the entrance channel:
The energetics (Q = Qrad + Qnu) of the reaction is also
provided in the header.
Q is computed from Audi & Wapstra mass table (Audi
G., Wapstra A.H., 1995, Nucl. Phys. A595, 409) or Goriely et al. mass table (Goriely S., Pearson J.M., Tondeur F., 2000, Atomic Data Nucl. Data Tables, in press), as the difference between
the mass excess in the entrance and exit chanels.
Qrad provides the radiative losses, i.e., Q - Qnu, where
Qnu is the energy possibly carried away by neutrinos.
The neutrino loss Qnu is computed according to Eqs. 1
and 2 of Fowler W.A., Caughlan G.R. & Zimmerman B.A. (1975, ARA&A
13, 69).
# 1 C 11 1 C 11 1 C 11 1 C 12 1 C 12 1 C 12 1 C 13 1 C 13 1 C 13 1 C 14 # + + + + + + + + + + # 1 PROT 1 PROT 0 OOOOO 1 PROT 1 PROT 1 PROT 1 PROT 1 PROT 1 PROT 1 PROT # = = = = = = = = = = # 0 OOOOO 1 HE 4 0 OOOOO 0 OOOOO 1 NEUT 1 HE 4 0 OOOOO 1 NEUT 1 HE 4 0 OOOOO # + + + + + + + + + + # 1 N 12 1 B 8 1 B 11 1 N 13 1 N 12 1 B 9 1 N 14 1 N 13 1 B 10 1 N 15 # # Qrad(MeV) .602 -7.406 1.401 1.944 -18.120 -7.552 7.551 -3.002 -4.062 10.208 # Qnu (MeV) .000 .000 .582 .000 .000 .000 .000 .000 .000 .000 # Type -- -- + -- -- -- -- -- -- -- # # T8 # .5000 .1826E-08 .1000E-98 .5663E-03 .1400E-07 .1000E-98 .1000E-98 .5530E-07 .1000E-24 .1000E-98 .5689E-07 1.0000 .2415E-05 .1000E-98 .5663E-03 .2180E-04 .1000E-98 .1000E-98 .8430E-04 .1000E-24 .1000E-98 .7857E-04 1.5000 .7791E-04 .1000E-98 .5663E-03 .8080E-03 .1000E-98 .1000E-98 .3000E-02 .1000E-24 .1000E-98 .2551E-02 2.0000 .7042E-03 .1000E-98 .5663E-03 .8660E-02 .1000E-98 .1000E-98 .2930E-01 .1000E-24 .1000E-98 .2332E-01 2.5000 .3457E-02 .1000E-98 .5663E-03 .5500E-01 .1000E-98 .1000E-98 .1540E+00 .1000E-24 .1134E-86 .1233E+00 3.0000 .1205E-01 .1000E-98 .5663E-03 .2780E+00 .1000E-98 .1000E-98 .5810E+00 .1000E-24 .5679E-72 .4930E+00 3.5000 .3377E-01 .1000E-98 .5663E-03 .1150E+01 .1000E-98 .1000E-98 .1960E+01 .1000E-24 .1141E-62 .1594E+01 4.0000 .8116E-01 .1816E-94 .5663E-03 .3810E+01 .1000E-98 .8882E-95 .6040E+01 .1000E-24 .2293E-53 .4289E+01 4.5000 .1739E+00 .1636E-83 .5663E-03 .1020E+02 .1000E-98 .1026E-84 .1690E+02 .1000E-24 .1063E-47 .9916E+01 5.0000 .3407E+00 .1007E-74 .5663E-03 .2280E+02 .1000E-98 .1184E-74 .4200E+02 .6390E-22 .4930E-42 .2030E+02 # # 1 C 14 1 C 14 1 C 15 1 C 15 1 C 15 1 C 15 1 N 13 1 N 13 1 N 13 1 N 13 # + + + + + + + + + + # 1 PROT 1 PROT 1 PROT 1 PROT 1 PROT 0 OOOOO 1 PROT 1 PROT 1 PROT 0 OOOOO # = = = = = = = = = = # 1 NEUT 1 HE 4 0 OOOOO 1 NEUT 1 HE 4 0 OOOOO 0 OOOOO 1 NEUT 1 HE 4 0 OOOOO # + + + + + + + + + + # 1 N 14 1 B 11 1 N 16 1 N 15 1 B 12 1 N 15 1 O 14 1 O 13 1 C 10 1 C 13 # # Qrad(MeV) -.625 -.784 11.479 8.990 1.368 4.708 4.628 -18.548 -5.490 1.508 # Qnu (MeV) .000 .000 .000 .000 .000 5.064 .000 .000 .000 .712 # Type -- -- -- -- -- + -- -- -- + # # T8 # .5000 .7413E-57 .4429E-98 .1000E-98 .1000E-98 .1000E-98 .2830E+00 .4620E-09 .1000E-98 .1000E-98 .1160E-02 ......................................
What is to be found in the log file?
The log file lists all bibliographical references available for the requested reactions (along with the date of inclusion of the library), and the reference selected for the given reaction.
1 1 C 11 ( 1 PROT , 0 OOOOO) 1 N 12 Number of rates available = 3 # Date Reference 1 0 WARNING: Not valid above T9 = 1!! Descouvemont P., Baraffe I ., 1990, Nucl.Phys. A514, 66 2 0 Wiescher M., Goerres J., Graff S., Buchmann L., Thielemann F .K., 1989, ApJ 343, 352 3 0 CF88 Ref. # 1 selected for reaction 1 C 11 ( 1 PROT , 0 OOOOO) 1 N 12 =============================================================================== 2 1 C 11 ( 1 PROT , 1 HE 4) 1 B 8 Data for computing inverse factor for B(b,a)A: Q(MeV) A(B) spin(B) A(b) g(b) Kronecker(B,b) stoe(B) stoe(b) -7.4060 11 1.5 1.0 2.0 .0 1 1 8 2.0 4.0 1.0 .0 1 1 A(A) spin(A) A(a) g(a) Kronecker(A,a) stoe(A) stoe(a) Number of rates available = 1 # Date Reference 1 240493 WARNING: Valid T9 < 0.8! Descouvemont P., Baraffe I., 1990, Nucl. Phys. A514, 66 Ref. # 1 selected for reaction 1 B 8 ( 1 HE 4, 1 PROT ) 1 C 11 =============================================================================== 3 1 C 11 ( 0 OOOOO, 0 OOOOO) 1 B 11
........................................................ ===============================================================================
1 1 C 11 ( 1 PROT , 0 OOOOO) 1 N 12 1 1 C 11 ( 1 PROT , 1 HE 4) 1 B 8 1 1 C 11 ( 0 OOOOO, 0 OOOOO) 1 B 11 1 1 C 12 ( 1 PROT , 0 OOOOO) 1 N 13 1 1 C 12 ( 1 PROT , 1 NEUT ) 1 N 12 1 1 C 12 ( 1 PROT , 1 HE 4) 1 B 9 1 1 C 13 ( 1 PROT , 0 OOOOO) 1 N 14 .........................
1 1 F 20 ( 1 PROT , 0 OOOOO) 1 NE 21 1 1 F 20 ( 1 PROT , 1 NEUT ) 1 NE 20 1 1 F 20 ( 1 PROT , 1 HE 4) 1 O 17 1 1 F 20 ( 0 OOOOO, 0 OOOOO) 1 NE 20