ENTRY C0488 20160321 C158C048800000001
SUBENT C0488001 20160321 C158C048800100001
BIB 10 24 C048800100002
TITLE Thick-target yields and astrophysical thermonuclear C048800100003
reaction rates: proton-induced reactions C048800100004
AUTHOR (N.A.Roughton,M.J.Fritts,R.J.Peterson,C.S.Zaidins, C048800100005
C.J.Hansen) C048800100006
REFERENCE (J,AND,23,177,197902) C048800100007
#doi:10.1016/0092-640X(79)90004-4 C048800100008
REL-REF (O,C0487001,N.A.Roughton+,J,AJ,205,302,1976) Data on C048800100009
30 reaction yields that are published in J,AND,23,177, C048800100010
197902 and missing in this entry. C048800100011
INSTITUTE (1USACLU) C048800100012
FACILITY (CYCLO,1USACLU) University of Colorado variable C048800100013
energy cyclotron facility. C048800100014
SAMPLE Targets were sufficiently thick to stop the beam, and C048800100015
assumed to be isotopically pure. C048800100016
METHOD (EXTB,SITA,ACTIV) C048800100017
DETECTOR (GELI) Ge(Li) detector, shielded by approximately 20 C048800100018
cm of lead on all sides to detect beta-delayed decay C048800100019
gammas or annihilation quanta. Detector calibration C048800100020
results: energy is within 3 keV and efficiency is C048800100021
within 5%. C048800100022
HISTORY (19990421C) C048800100023
(20030625A) Reference corrected, BIB update. C048800100024
(20160321A) BP: Updated the entry to the current C048800100025
standards, added doi, missing reaction rates data. C048800100026
ENDBIB 24 0 C048800100027
NOCOMMON 0 0 C048800100028
ENDSUBENT 27 0 C048800199999
SUBENT C0488002 20160321 C158C048800200001
BIB 3 10 C048800200002
REACTION (7-N-14(P,G)8-O-15,,PY,,TT) C048800200003
ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C048800200004
. either statistical, due to number of gamma counts, C048800200005
. or set to 7% due to uncertainties in of about 5% in C048800200006
bombardment parameters such as current integration C048800200007
and 5 % in counting due to source location, etc., C048800200008
added in quadrature. C048800200009
(ERR-1) Bombardment parameters. C048800200010
(ERR-2) Source location. C048800200011
STATUS (TABLE) Table II, page 184. C048800200012
ENDBIB 10 0 C048800200013
COMMON 2 3 C048800200014
ERR-1 ERR-2 C048800200015
PER-CENT PER-CENT C048800200016
5.0 5.0 C048800200017
ENDCOMMON 3 0 C048800200018
DATA 3 13 C048800200019
EN-CM DATA DATA-ERR C048800200020
MEV PRD/INC PRD/INC C048800200021
0.356 3.70E-11 1.90E-11 C048800200022
0.665 4.50E-11 9.00E-12 C048800200023
0.844 8.50E-11 2.20E-11 C048800200024
1.102 8.30E-10 1.20E-10 C048800200025
1.282 1.20E-09 4.00E-10 C048800200026
1.410 1.50E-09 2.00E-10 C048800200027
1.462 1.25E-09 1.30E-10 C048800200028
1.550 1.39E-09 1.00E-10 C048800200029
1.651 1.67E-09 2.00E-10 C048800200030
1.932 3.10E-09 3.00E-10 C048800200031
2.226 6.80E-09 5.00E-10 C048800200032
2.425 1.20E-08 1.00E-09 C048800200033
2.596 1.25E-08 1.50E-09 C048800200034
ENDDATA 15 0 C048800200035
ENDSUBENT 34 0 C048800299999
SUBENT C0488003 20160321 C158C048800300001
BIB 3 10 C048800300002
REACTION (38-SR-87(P,G)39-Y-88,,PY,,TT) C048800300003
ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C048800300004
. either statistical, due to number of gamma counts, C048800300005
. or set to 7% due to uncertainties in of about 5% in C048800300006
bombardment parameters such as current integration C048800300007
and 5 % in counting due to source location, etc., C048800300008
added in quadrature. C048800300009
(ERR-1) Bombardment parameters. C048800300010
(ERR-2) Source location. C048800300011
STATUS (TABLE) Table II, page 185. C048800300012
ENDBIB 10 0 C048800300013
COMMON 2 3 C048800300014
ERR-1 ERR-2 C048800300015
PER-CENT PER-CENT C048800300016
5.0 5.0 C048800300017
ENDCOMMON 3 0 C048800300018
DATA 3 7 C048800300019
EN-CM DATA DATA-ERR C048800300020
MEV PRD/INC PRD/INC C048800300021
2.570 4.30E-07 1.40E-07 C048800300022
2.780 1.10E-06 3.00E-07 C048800300023
2.990 7.30E-07 2.50E-07 C048800300024
3.310 1.70E-06 4.00E-07 C048800300025
3.350 2.20E-06 4.00E-07 C048800300026
3.900 5.00E-06 1.70E-06 C048800300027
4.240 9.80E-06 2.40E-06 C048800300028
ENDDATA 9 0 C048800300029
ENDSUBENT 28 0 C048800399999
SUBENT C0488004 20160321 C158C048800400001
BIB 3 10 C048800400002
REACTION (40-ZR-90(P,G)41-NB-91-M,,PY,,TT) C048800400003
ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C048800400004
. either statistical, due to number of gamma counts, C048800400005
. or set to 7% due to uncertainties in of about 5% in C048800400006
bombardment parameters such as current integration C048800400007
and 5 % in counting due to source location, etc., C048800400008
added in quadrature. C048800400009
(ERR-1) Bombardment parameters. C048800400010
(ERR-2) Source location. C048800400011
STATUS (TABLE) Table II, page 185. C048800400012
ENDBIB 10 0 C048800400013
COMMON 2 3 C048800400014
ERR-1 ERR-2 C048800400015
PER-CENT PER-CENT C048800400016
5.0 5.0 C048800400017
ENDCOMMON 3 0 C048800400018
DATA 3 15 C048800400019
EN-CM DATA DATA-ERR C048800400020
MEV PRD/INC PRD/INC C048800400021
1.750 3.00E-10 2.00E-10 C048800400022
2.047 3.10E-10 2.90E-10 C048800400023
2.091 9.00E-10 3.00E-10 C048800400024
2.569 3.70E-09 1.00E-09 C048800400025
2.786 5.10E-09 8.00E-10 C048800400026
3.041 1.72E-08 2.00E-09 C048800400027
3.309 3.70E-08 3.00E-09 C048800400028
3.770 1.20E-07 1.10E-08 C048800400029
4.245 2.65E-07 2.00E-08 C048800400030
4.621 5.50E-07 4.00E-08 C048800400031
5.180 1.02E-06 8.00E-08 C048800400032
5.368 1.45E-06 1.01E-07 C048800400033
5.600 2.41E-06 2.00E-07 C048800400034
6.015 3.35E-06 2.34E-07 C048800400035
6.426 5.30E-06 4.10E-07 C048800400036
ENDDATA 17 0 C048800400037
ENDSUBENT 36 0 C048800499999
SUBENT C0488005 20160321 C158C048800500001
BIB 3 10 C048800500002
REACTION (46-PD-102(P,G)47-AG-103,,PY,,TT) C048800500003
ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C048800500004
. either statistical, due to number of gamma counts, C048800500005
. or set to 7% due to uncertainties in of about 5% in C048800500006
bombardment parameters such as current integration C048800500007
and 5 % in counting due to source location, etc., C048800500008
added in quadrature. C048800500009
(ERR-1) Bombardment parameters. C048800500010
(ERR-2) Source location. C048800500011
STATUS (TABLE) Table II, page 186. C048800500012
ENDBIB 10 0 C048800500013
COMMON 2 3 C048800500014
ERR-1 ERR-2 C048800500015
PER-CENT PER-CENT C048800500016
5.0 5.0 C048800500017
ENDCOMMON 3 0 C048800500018
DATA 3 15 C048800500019
EN-CM DATA DATA-ERR C048800500020
MEV PRD/INC PRD/INC C048800500021
2.575 6.54E-10 1.50E-10 C048800500022
2.985 5.39E-09 3.77E-10 C048800500023
3.483 2.50E-08 1.75E-09 C048800500024
3.535 2.15E-08 3.00E-09 C048800500025
3.842 7.37E-08 2.00E-08 C048800500026
3.976 1.30E-07 9.10E-09 C048800500027
4.298 1.31E-07 9.17E-09 C048800500028
4.545 3.21E-07 2.25E-08 C048800500029
4.652 5.51E-07 3.86E-08 C048800500030
4.678 5.29E-07 3.70E-08 C048800500031
5.113 7.64E-07 7.60E-08 C048800500032
5.223 8.00E-07 4.00E-07 C048800500033
5.541 1.53E-06 5.00E-07 C048800500034
6.298 4.60E-06 6.09E-06 C048800500035
6.770 8.36E-06 1.20E-06 C048800500036
ENDDATA 17 0 C048800500037
ENDSUBENT 36 0 C048800599999
SUBENT C0488006 20160321 C158C048800600001
BIB 3 10 C048800600002
REACTION (48-CD-106(P,G)49-IN-107,,PY,,TT) C048800600003
ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C048800600004
. either statistical, due to number of gamma counts, C048800600005
. or set to 7% due to uncertainties in of about 5% in C048800600006
bombardment parameters such as current integration C048800600007
and 5 % in counting due to source location, etc., C048800600008
added in quadrature. C048800600009
(ERR-1) Bombardment parameters. C048800600010
(ERR-2) Source location. C048800600011
STATUS (TABLE) Table II, page 186. C048800600012
ENDBIB 10 0 C048800600013
COMMON 2 3 C048800600014
ERR-1 ERR-2 C048800600015
PER-CENT PER-CENT C048800600016
5.0 5.0 C048800600017
ENDCOMMON 3 0 C048800600018
DATA 3 12 C048800600019
EN-CM DATA DATA-ERR C048800600020
MEV PRD/INC PRD/INC C048800600021
3.000 1.93E-09 3.70E-10 C048800600022
3.360 8.74E-09 1.46E-09 C048800600023
3.530 9.89E-09 1.71E-09 C048800600024
3.830 2.02E-08 2.80E-09 C048800600025
3.910 4.91E-08 6.80E-09 C048800600026
4.230 5.53E-08 7.40E-09 C048800600027
4.350 1.17E-07 1.54E-08 C048800600028
4.490 1.25E-07 1.70E-08 C048800600029
4.600 2.18E-07 2.90E-08 C048800600030
4.660 2.48E-07 3.30E-08 C048800600031
4.950 2.92E-07 3.90E-08 C048800600032
5.000 4.18E-07 5.50E-08 C048800600033
ENDDATA 14 0 C048800600034
ENDSUBENT 33 0 C048800699999
SUBENT C0488007 20160321 C158C048800700001
BIB 3 10 C048800700002
REACTION (48-CD-108(P,G)49-IN-109,,PY,,TT) C048800700003
ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C048800700004
. either statistical, due to number of gamma counts, C048800700005
. or set to 7% due to uncertainties in of about 5% in C048800700006
bombardment parameters such as current integration C048800700007
and 5 % in counting due to source location, etc., C048800700008
added in quadrature. C048800700009
(ERR-1) Bombardment parameters. C048800700010
(ERR-2) Source location. C048800700011
STATUS (TABLE) Table II, page 186. C048800700012
ENDBIB 10 0 C048800700013
COMMON 2 3 C048800700014
ERR-1 ERR-2 C048800700015
PER-CENT PER-CENT C048800700016
5.0 5.0 C048800700017
ENDCOMMON 3 0 C048800700018
DATA 3 12 C048800700019
EN-CM DATA DATA-ERR C048800700020
MEV PRD/INC PRD/INC C048800700021
3.000 4.39E-09 8.30E-10 C048800700022
3.360 1.35E-08 2.20E-09 C048800700023
3.530 1.31E-08 2.20E-09 C048800700024
3.830 5.25E-08 6.90E-09 C048800700025
3.910 7.42E-08 9.90E-09 C048800700026
4.230 1.23E-07 1.60E-08 C048800700027
4.350 1.71E-07 2.20E-08 C048800700028
4.490 2.28E-07 3.00E-08 C048800700029
4.600 3.69E-07 4.90E-08 C048800700030
4.660 3.93E-07 5.10E-08 C048800700031
4.950 5.28E-07 6.80E-08 C048800700032
5.000 1.06E-06 1.38E-07 C048800700033
ENDDATA 14 0 C048800700034
ENDSUBENT 33 0 C048800799999
SUBENT C0488008 20160321 C158C048800800001
BIB 3 10 C048800800002
REACTION (48-CD-114(P,G)49-IN-115-M,,PY,,TT) C048800800003
ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C048800800004
. either statistical, due to number of gamma counts, C048800800005
. or set to 7% due to uncertainties in of about 5% in C048800800006
bombardment parameters such as current integration C048800800007
and 5 % in counting due to source location, etc., C048800800008
added in quadrature. C048800800009
(ERR-1) Bombardment parameters. C048800800010
(ERR-2) Source location. C048800800011
STATUS (TABLE) Table II, page 186. C048800800012
ENDBIB 10 0 C048800800013
COMMON 2 3 C048800800014
ERR-1 ERR-2 C048800800015
PER-CENT PER-CENT C048800800016
5.0 5.0 C048800800017
ENDCOMMON 3 0 C048800800018
DATA 3 13 C048800800019
EN-CM DATA DATA-ERR C048800800020
MEV PRD/INC PRD/INC C048800800021
3.000 8.40E-10 1.20E-10 C048800800022
3.060 1.26E-09 1.90E-10 C048800800023
3.360 1.98E-09 2.70E-10 C048800800024
3.530 2.52E-09 3.40E-10 C048800800025
3.830 4.22E-09 4.70E-10 C048800800026
3.910 6.28E-09 9.30E-10 C048800800027
4.230 6.91E-09 7.70E-10 C048800800028
4.350 9.74E-09 1.20E-09 C048800800029
4.490 1.18E-08 1.60E-09 C048800800030
4.600 1.59E-08 1.90E-09 C048800800031
4.660 1.82E-08 2.40E-09 C048800800032
4.950 1.99E-08 2.10E-09 C048800800033
5.000 3.20E-08 5.70E-09 C048800800034
ENDDATA 15 0 C048800800035
ENDSUBENT 34 0 C048800899999
SUBENT C0488009 20160321 C158C048800900001
BIB 3 10 C048800900002
REACTION (48-CD-116(P,G)49-IN-117-M,,PY,,TT) C048800900003
ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C048800900004
. either statistical, due to number of gamma counts, C048800900005
. or set to 7% due to uncertainties in of about 5% in C048800900006
bombardment parameters such as current integration C048800900007
and 5 % in counting due to source location, etc., C048800900008
added in quadrature. C048800900009
(ERR-1) Bombardment parameters. C048800900010
(ERR-2) Source location. C048800900011
STATUS (TABLE) Table II, page 186. C048800900012
ENDBIB 10 0 C048800900013
COMMON 2 3 C048800900014
ERR-1 ERR-2 C048800900015
PER-CENT PER-CENT C048800900016
5.0 5.0 C048800900017
ENDCOMMON 3 0 C048800900018
DATA 3 10 C048800900019
EN-CM DATA DATA-ERR C048800900020
MEV PRD/INC PRD/INC C048800900021
3.000 2.00E-11 2.70E-11 C048800900022
3.360 2.04E-10 9.50E-11 C048800900023
3.530 1.96E-10 1.07E-10 C048800900024
3.830 4.40E-10 1.30E-10 C048800900025
3.910 8.10E-10 2.90E-10 C048800900026
4.230 9.90E-10 2.30E-10 C048800900027
4.350 1.90E-09 7.00E-10 C048800900028
4.490 2.30E-09 8.10E-10 C048800900029
4.660 4.70E-09 1.10E-09 C048800900030
4.950 5.80E-09 2.20E-09 C048800900031
ENDDATA 12 0 C048800900032
ENDSUBENT 31 0 C048800999999
SUBENT C0488010 20160321 C158C048801000001
BIB 3 10 C048801000002
REACTION (50-SN-112(P,G)51-SB-113,,PY,,TT) C048801000003
ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C048801000004
. either statistical, due to number of gamma counts, C048801000005
. or set to 7% due to uncertainties in of about 5% in C048801000006
bombardment parameters such as current integration C048801000007
and 5 % in counting due to source location, etc., C048801000008
added in quadrature. C048801000009
(ERR-1) Bombardment parameters. C048801000010
(ERR-2) Source location. C048801000011
STATUS (TABLE) Table II, page 186. C048801000012
ENDBIB 10 0 C048801000013
COMMON 2 3 C048801000014
ERR-1 ERR-2 C048801000015
PER-CENT PER-CENT C048801000016
5.0 5.0 C048801000017
ENDCOMMON 3 0 C048801000018
DATA 3 4 C048801000019
EN-CM DATA DATA-ERR C048801000020
MEV PRD/INC PRD/INC C048801000021
2.987 3.13E-09 4.80E-10 C048801000022
3.538 3.25E-08 4.10E-09 C048801000023
3.845 7.66E-08 7.00E-09 C048801000024
3.979 5.10E-08 2.52E-08 C048801000025
ENDDATA 6 0 C048801000026
ENDSUBENT 25 0 C048801099999
SUBENT C0488011 20160321 C158C048801100001
BIB 3 10 C048801100002
REACTION (62-SM-144(P,G)63-EU-145,,PY,,TT) C048801100003
ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C048801100004
. either statistical, due to number of gamma counts, C048801100005
. or set to 7% due to uncertainties in of about 5% in C048801100006
bombardment parameters such as current integration C048801100007
and 5 % in counting due to source location, etc., C048801100008
added in quadrature. C048801100009
(ERR-1) Bombardment parameters. C048801100010
(ERR-2) Source location. C048801100011
STATUS (TABLE) Table II, page 186. C048801100012
ENDBIB 10 0 C048801100013
COMMON 2 3 C048801100014
ERR-1 ERR-2 C048801100015
PER-CENT PER-CENT C048801100016
5.0 5.0 C048801100017
ENDCOMMON 3 0 C048801100018
DATA 3 11 C048801100019
EN-CM DATA DATA-ERR C048801100020
MEV PRD/INC PRD/INC C048801100021
3.320 1.50E-09 1.50E-09 C048801100022
3.379 2.10E-09 5.00E-10 C048801100023
3.908 9.25E-09 1.50E-09 C048801100024
4.262 1.06E-08 2.90E-09 C048801100025
4.616 1.30E-08 2.90E-09 C048801100026
5.018 3.28E-08 7.20E-09 C048801100027
5.200 4.82E-08 9.60E-09 C048801100028
5.389 5.54E-08 7.20E-09 C048801100029
5.649 1.49E-07 2.40E-08 C048801100030
6.320 6.84E-07 9.60E-08 C048801100031
6.792 1.05E-06 1.90E-07 C048801100032
ENDDATA 13 0 C048801100033
ENDSUBENT 32 0 C048801199999
SUBENT C0488012 20160321 C158C048801200001
BIB 3 10 C048801200002
REACTION (38-SR-87(P,N)39-Y-87,,PY,,TT) C048801200003
ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C048801200004
. either statistical, due to number of gamma counts, C048801200005
. or set to 7% due to uncertainties in of about 5% in C048801200006
bombardment parameters such as current integration C048801200007
and 5 % in counting due to source location, etc., C048801200008
added in quadrature. C048801200009
(ERR-1) Bombardment parameters. C048801200010
(ERR-2) Source location. C048801200011
STATUS (TABLE) Table II, page 187. C048801200012
ENDBIB 10 0 C048801200013
COMMON 2 3 C048801200014
ERR-1 ERR-2 C048801200015
PER-CENT PER-CENT C048801200016
5.0 5.0 C048801200017
ENDCOMMON 3 0 C048801200018
DATA 3 12 C048801200019
EN-CM DATA DATA-ERR C048801200020
MEV PRD/INC PRD/INC C048801200021
2.570 1.10E-08 1.00E-09 C048801200022
2.780 2.20E-08 2.00E-09 C048801200023
2.990 4.60E-08 7.00E-09 C048801200024
3.310 5.70E-08 1.60E-08 C048801200025
3.350 1.20E-07 1.00E-08 C048801200026
3.900 6.40E-07 4.48E-08 C048801200027
4.240 1.30E-06 1.00E-07 C048801200028
4.590 2.50E-06 5.00E-07 C048801200029
4.990 4.00E-06 1.00E-06 C048801200030
5.100 7.20E-06 7.00E-07 C048801200031
5.180 7.30E-06 1.50E-06 C048801200032
5.620 1.30E-05 1.00E-06 C048801200033
ENDDATA 14 0 C048801200034
ENDSUBENT 33 0 C048801299999
SUBENT C0488013 20160321 C158C048801300001
BIB 3 10 C048801300002
REACTION (38-SR-88(P,N)39-Y-88,,PY,,TT) C048801300003
ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C048801300004
. either statistical, due to number of gamma counts, C048801300005
. or set to 7% due to uncertainties in of about 5% in C048801300006
bombardment parameters such as current integration C048801300007
and 5 % in counting due to source location, etc., C048801300008
added in quadrature. C048801300009
(ERR-1) Bombardment parameters. C048801300010
(ERR-2) Source location. C048801300011
STATUS (TABLE) Table II, page 187. C048801300012
ENDBIB 10 0 C048801300013
COMMON 2 3 C048801300014
ERR-1 ERR-2 C048801300015
PER-CENT PER-CENT C048801300016
5.0 5.0 C048801300017
ENDCOMMON 3 0 C048801300018
DATA 3 5 C048801300019
EN-CM DATA DATA-ERR C048801300020
MEV PRD/INC PRD/INC C048801300021
4.590 8.00E-08 7.50E-08 C048801300022
4.990 5.20E-06 4.00E-07 C048801300023
5.100 9.00E-06 1.00E-06 C048801300024
5.180 9.70E-06 1.00E-06 C048801300025
5.620 3.90E-05 2.73E-06 C048801300026
ENDDATA 7 0 C048801300027
ENDSUBENT 26 0 C048801399999
SUBENT C0488014 20160321 C158C048801400001
BIB 3 10 C048801400002
REACTION (40-ZR-94(P,N)41-NB-94-M,,PY,,TT) C048801400003
ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C048801400004
. either statistical, due to number of gamma counts, C048801400005
. or set to 7% due to uncertainties in of about 5% in C048801400006
bombardment parameters such as current integration C048801400007
and 5 % in counting due to source location, etc., C048801400008
added in quadrature. C048801400009
(ERR-1) Bombardment parameters. C048801400010
(ERR-2) Source location. C048801400011
STATUS (TABLE) Table II, page 187. C048801400012
ENDBIB 10 0 C048801400013
COMMON 2 3 C048801400014
ERR-1 ERR-2 C048801400015
PER-CENT PER-CENT C048801400016
5.0 5.0 C048801400017
ENDCOMMON 3 0 C048801400018
DATA 3 13 C048801400019
EN-CM DATA DATA-ERR C048801400020
MEV PRD/INC PRD/INC C048801400021
3.056 1.67E-07 1.67E-08 C048801400022
3.480 6.73E-07 6.73E-08 C048801400023
3.530 8.24E-07 8.24E-08 C048801400024
3.840 2.14E-06 2.14E-07 C048801400025
3.972 2.62E-06 2.62E-07 C048801400026
4.294 3.98E-06 3.98E-07 C048801400027
4.640 7.89E-06 7.89E-07 C048801400028
4.716 1.51E-05 1.51E-06 C048801400029
4.720 1.51E-05 1.51E-06 C048801400030
4.942 1.89E-05 1.89E-06 C048801400031
5.220 3.31E-05 3.31E-06 C048801400032
5.536 5.82E-05 5.82E-06 C048801400033
5.953 7.42E-05 7.42E-06 C048801400034
ENDDATA 15 0 C048801400035
ENDSUBENT 34 0 C048801499999
SUBENT C0488015 20160321 C158C048801500001
BIB 3 10 C048801500002
REACTION (40-ZR-96(P,N)41-NB-96,,PY,,TT) C048801500003
ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C048801500004
. either statistical, due to number of gamma counts, C048801500005
. or set to 7% due to uncertainties in of about 5% in C048801500006
bombardment parameters such as current integration C048801500007
and 5 % in counting due to source location, etc., C048801500008
added in quadrature. C048801500009
(ERR-1) Bombardment parameters. C048801500010
(ERR-2) Source location. C048801500011
STATUS (TABLE) Table II, page 187. C048801500012
ENDBIB 10 0 C048801500013
COMMON 2 3 C048801500014
ERR-1 ERR-2 C048801500015
PER-CENT PER-CENT C048801500016
5.0 5.0 C048801500017
ENDCOMMON 3 0 C048801500018
DATA 3 12 C048801500019
EN-CM DATA DATA-ERR C048801500020
MEV PRD/INC PRD/INC C048801500021
3.057 4.48E-08 4.48E-09 C048801500022
3.480 2.35E-07 2.35E-08 C048801500023
3.530 2.71E-07 2.71E-08 C048801500024
3.840 5.37E-07 5.37E-08 C048801500025
3.974 1.01E-06 1.01E-07 C048801500026
4.295 1.88E-06 1.88E-07 C048801500027
4.640 3.53E-06 3.53E-07 C048801500028
4.720 4.54E-06 4.54E-07 C048801500029
4.945 6.80E-06 6.80E-07 C048801500030
5.220 1.42E-05 1.42E-06 C048801500031
5.537 2.26E-05 2.26E-06 C048801500032
5.954 3.69E-05 3.69E-06 C048801500033
ENDDATA 14 0 C048801500034
ENDSUBENT 33 0 C048801599999
SUBENT C0488016 20160321 C158C048801600001
BIB 3 10 C048801600002
REACTION (46-PD-104(P,N)47-AG-104,,PY,,TT) C048801600003
ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C048801600004
. either statistical, due to number of gamma counts, C048801600005
. or set to 7% due to uncertainties in of about 5% in C048801600006
bombardment parameters such as current integration C048801600007
and 5 % in counting due to source location, etc., C048801600008
added in quadrature. C048801600009
(ERR-1) Bombardment parameters. C048801600010
(ERR-2) Source location. C048801600011
STATUS (TABLE) Table II, page 187. C048801600012
ENDBIB 10 0 C048801600013
COMMON 2 3 C048801600014
ERR-1 ERR-2 C048801600015
PER-CENT PER-CENT C048801600016
5.0 5.0 C048801600017
ENDCOMMON 3 0 C048801600018
DATA 3 4 C048801600019
EN-CM DATA DATA-ERR C048801600020
MEV PRD/INC PRD/INC C048801600021
5.118 6.90E-09 1.08E-09 C048801600022
5.225 2.75E-07 4.13E-08 C048801600023
5.542 8.34E-07 5.84E-08 C048801600024
5.958 4.46E-06 6.69E-07 C048801600025
ENDDATA 6 0 C048801600026
ENDSUBENT 25 0 C048801699999
SUBENT C0488017 20160321 C158C048801700001
BIB 3 10 C048801700002
REACTION (46-PD-105(P,N)47-AG-105,,PY,,TT) C048801700003
ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C048801700004
. either statistical, due to number of gamma counts, C048801700005
. or set to 7% due to uncertainties in of about 5% in C048801700006
bombardment parameters such as current integration C048801700007
and 5 % in counting due to source location, etc., C048801700008
added in quadrature. C048801700009
(ERR-1) Bombardment parameters. C048801700010
(ERR-2) Source location. C048801700011
STATUS (TABLE) Table II, page 187. C048801700012
ENDBIB 10 0 C048801700013
COMMON 2 3 C048801700014
ERR-1 ERR-2 C048801700015
PER-CENT PER-CENT C048801700016
5.0 5.0 C048801700017
ENDCOMMON 3 0 C048801700018
DATA 3 11 C048801700019
EN-CM DATA DATA-ERR C048801700020
MEV PRD/INC PRD/INC C048801700021
3.536 5.09E-08 7.63E-09 C048801700022
3.843 1.32E-07 1.98E-08 C048801700023
3.980 2.56E-07 6.00E-08 C048801700024
4.300 5.72E-07 8.58E-08 C048801700025
4.547 1.26E-06 1.26E-07 C048801700026
4.679 1.68E-06 1.68E-07 C048801700027
4.954 2.33E-06 2.33E-07 C048801700028
5.114 4.20E-06 4.20E-07 C048801700029
5.225 4.62E-06 4.62E-07 C048801700030
5.542 8.49E-06 8.49E-07 C048801700031
5.960 1.36E-05 1.36E-06 C048801700032
ENDDATA 13 0 C048801700033
ENDSUBENT 32 0 C048801799999
SUBENT C0488018 20160321 C158C048801800001
BIB 3 10 C048801800002
REACTION (46-PD-106(P,N)47-AG-106,,PY,,TT) C048801800003
ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C048801800004
. either statistical, due to number of gamma counts, C048801800005
. or set to 7% due to uncertainties in of about 5% in C048801800006
bombardment parameters such as current integration C048801800007
and 5 % in counting due to source location, etc., C048801800008
added in quadrature. C048801800009
(ERR-1) Bombardment parameters. C048801800010
(ERR-2) Source location. C048801800011
STATUS (TABLE) Table II, page 187. C048801800012
ENDBIB 10 0 C048801800013
COMMON 2 3 C048801800014
ERR-1 ERR-2 C048801800015
PER-CENT PER-CENT C048801800016
5.0 5.0 C048801800017
ENDCOMMON 3 0 C048801800018
DATA 3 7 C048801800019
EN-CM DATA DATA-ERR C048801800020
MEV PRD/INC PRD/INC C048801800021
3.977 1.74E-07 2.61E-08 C048801800022
4.299 6.14E-07 9.21E-08 C048801800023
4.547 3.48E-06 5.43E-07 C048801800024
4.954 6.47E-06 9.70E-07 C048801800025
5.226 9.83E-06 1.95E-06 C048801800026
5.543 2.93E-05 5.10E-06 C048801800027
5.960 5.14E-05 5.40E-06 C048801800028
ENDDATA 9 0 C048801800029
ENDSUBENT 28 0 C048801899999
SUBENT C0488019 20160321 C158C048801900001
BIB 3 10 C048801900002
REACTION (46-PD-106(P,N)47-AG-106-M,,PY,,TT) C048801900003
ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C048801900004
. either statistical, due to number of gamma counts, C048801900005
. or set to 7% due to uncertainties in of about 5% in C048801900006
bombardment parameters such as current integration C048801900007
and 5 % in counting due to source location, etc., C048801900008
added in quadrature. C048801900009
(ERR-1) Bombardment parameters. C048801900010
(ERR-2) Source location. C048801900011
STATUS (TABLE) Table II, page 187. C048801900012
ENDBIB 10 0 C048801900013
COMMON 2 3 C048801900014
ERR-1 ERR-2 C048801900015
PER-CENT PER-CENT C048801900016
5.0 5.0 C048801900017
ENDCOMMON 3 0 C048801900018
DATA 3 8 C048801900019
EN-CM DATA DATA-ERR C048801900020
MEV PRD/INC PRD/INC C048801900021
3.977 6.90E-10 6.20E-10 C048801900022
4.547 4.27E-08 6.40E-09 C048801900023
4.679 2.20E-08 7.50E-09 C048801900024
4.954 3.64E-08 1.25E-08 C048801900025
5.114 1.29E-07 2.50E-08 C048801900026
5.225 7.90E-08 1.25E-08 C048801900027
5.543 1.32E-07 1.88E-08 C048801900028
5.959 4.02E-07 6.03E-08 C048801900029
ENDDATA 10 0 C048801900030
ENDSUBENT 29 0 C048801999999
SUBENT C0488020 20160321 C158C048802000001
BIB 3 10 C048802000002
REACTION (48-CD-116(P,N)49-IN-116-M,,PY,,TT) C048802000003
ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C048802000004
. either statistical, due to number of gamma counts, C048802000005
. or set to 7% due to uncertainties in of about 5% in C048802000006
bombardment parameters such as current integration C048802000007
and 5 % in counting due to source location, etc., C048802000008
added in quadrature. C048802000009
(ERR-1) Bombardment parameters. C048802000010
(ERR-2) Source location. C048802000011
STATUS (TABLE) Table II, page 187. C048802000012
ENDBIB 10 0 C048802000013
COMMON 2 3 C048802000014
ERR-1 ERR-2 C048802000015
PER-CENT PER-CENT C048802000016
5.0 5.0 C048802000017
ENDCOMMON 3 0 C048802000018
DATA 3 12 C048802000019
EN-CM DATA DATA-ERR C048802000020
MEV PRD/INC PRD/INC C048802000021
3.000 8.23E-10 2.34E-10 C048802000022
3.360 5.05E-09 9.40E-10 C048802000023
3.530 5.91E-09 9.90E-10 C048802000024
3.830 2.05E-08 3.00E-09 C048802000025
3.910 3.65E-08 5.50E-09 C048802000026
4.230 6.48E-08 9.50E-09 C048802000027
4.350 1.18E-07 1.70E-08 C048802000028
4.490 1.47E-07 2.10E-08 C048802000029
4.610 2.60E-07 3.80E-08 C048802000030
4.660 2.99E-07 5.70E-08 C048802000031
4.950 4.28E-07 6.20E-08 C048802000032
5.000 8.43E-07 1.32E-07 C048802000033
ENDDATA 14 0 C048802000034
ENDSUBENT 33 0 C048802099999
SUBENT C0488021 20160321 C158C048802100001
BIB 3 10 C048802100002
REACTION (50-SN-115(P,N)51-SB-115,,PY,,TT) C048802100003
ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C048802100004
. either statistical, due to number of gamma counts, C048802100005
. or set to 7% due to uncertainties in of about 5% in C048802100006
bombardment parameters such as current integration C048802100007
and 5 % in counting due to source location, etc., C048802100008
added in quadrature. C048802100009
(ERR-1) Bombardment parameters. C048802100010
(ERR-2) Source location. C048802100011
STATUS (TABLE) Table II, page 187. C048802100012
ENDBIB 10 0 C048802100013
COMMON 2 3 C048802100014
ERR-1 ERR-2 C048802100015
PER-CENT PER-CENT C048802100016
5.0 5.0 C048802100017
ENDCOMMON 3 0 C048802100018
DATA 3 4 C048802100019
EN-CM DATA DATA-ERR C048802100020
MEV PRD/INC PRD/INC C048802100021
4.683 2.42E-07 3.40E-08 C048802100022
5.118 1.35E-06 2.00E-07 C048802100023
5.547 2.80E-06 4.20E-07 C048802100024
5.964 1.12E-05 1.68E-06 C048802100025
ENDDATA 6 0 C048802100026
ENDSUBENT 25 0 C048802199999
SUBENT C0488022 20160321 C158C048802200001
BIB 3 10 C048802200002
REACTION (50-SN-117(P,N)51-SB-117,,PY,,TT) C048802200003
ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C048802200004
. either statistical, due to number of gamma counts, C048802200005
. or set to 7% due to uncertainties in of about 5% in C048802200006
bombardment parameters such as current integration C048802200007
and 5 % in counting due to source location, etc., C048802200008
added in quadrature. C048802200009
(ERR-1) Bombardment parameters. C048802200010
(ERR-2) Source location. C048802200011
STATUS (TABLE) Table II, page 187. C048802200012
ENDBIB 10 0 C048802200013
COMMON 2 3 C048802200014
ERR-1 ERR-2 C048802200015
PER-CENT PER-CENT C048802200016
5.0 5.0 C048802200017
ENDCOMMON 3 0 C048802200018
DATA 3 11 C048802200019
EN-CM DATA DATA-ERR C048802200020
MEV PRD/INC PRD/INC C048802200021
2.988 4.34E-09 6.51E-10 C048802200022
3.539 3.01E-08 4.50E-09 C048802200023
3.847 8.20E-08 1.23E-08 C048802200024
4.302 3.01E-07 4.50E-08 C048802200025
4.551 9.80E-07 1.47E-07 C048802200026
4.683 1.50E-06 2.25E-07 C048802200027
4.958 1.72E-06 2.58E-07 C048802200028
5.119 3.78E-06 5.67E-07 C048802200029
5.230 4.58E-06 6.87E-07 C048802200030
5.547 7.27E-06 1.09E-06 C048802200031
5.965 1.45E-05 2.18E-06 C048802200032
ENDDATA 13 0 C048802200033
ENDSUBENT 32 0 C048802299999
SUBENT C0488023 20160321 C158C048802300001
BIB 3 10 C048802300002
REACTION (50-SN-120(P,N)51-SB-120,,PY,,TT) C048802300003
ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C048802300004
. either statistical, due to number of gamma counts, C048802300005
. or set to 7% due to uncertainties in of about 5% in C048802300006
bombardment parameters such as current integration C048802300007
and 5 % in counting due to source location, etc., C048802300008
added in quadrature. C048802300009
(ERR-1) Bombardment parameters. C048802300010
(ERR-2) Source location. C048802300011
STATUS (TABLE) Table II, page 188. C048802300012
ENDBIB 10 0 C048802300013
COMMON 2 3 C048802300014
ERR-1 ERR-2 C048802300015
PER-CENT PER-CENT C048802300016
5.0 5.0 C048802300017
ENDCOMMON 3 0 C048802300018
DATA 3 9 C048802300019
EN-CM DATA DATA-ERR C048802300020
MEV PRD/INC PRD/INC C048802300021
3.540 7.00E-09 1.05E-09 C048802300022
3.848 3.89E-08 5.83E-09 C048802300023
3.982 8.67E-08 1.30E-08 C048802300024
4.304 1.57E-07 2.30E-08 C048802300025
4.552 5.75E-07 8.63E-08 C048802300026
4.685 9.66E-07 6.76E-08 C048802300027
5.120 2.53E-06 3.79E-07 C048802300028
5.548 4.69E-06 7.04E-07 C048802300029
5.966 1.03E-05 1.55E-06 C048802300030
ENDDATA 11 0 C048802300031
ENDSUBENT 30 0 C048802399999
SUBENT C0488024 20160321 C158C048802400001
BIB 3 10 C048802400002
REACTION (50-SN-122(P,N)51-SB-122,,PY,,TT) C048802400003
ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C048802400004
. either statistical, due to number of gamma counts, C048802400005
. or set to 7% due to uncertainties in of about 5% in C048802400006
bombardment parameters such as current integration C048802400007
and 5 % in counting due to source location, etc., C048802400008
added in quadrature. C048802400009
(ERR-1) Bombardment parameters. C048802400010
(ERR-2) Source location. C048802400011
STATUS (TABLE) Table II, page 188. C048802400012
ENDBIB 10 0 C048802400013
COMMON 2 3 C048802400014
ERR-1 ERR-2 C048802400015
PER-CENT PER-CENT C048802400016
5.0 5.0 C048802400017
ENDCOMMON 3 0 C048802400018
DATA 3 8 C048802400019
EN-CM DATA DATA-ERR C048802400020
MEV PRD/INC PRD/INC C048802400021
3.850 7.77E-08 1.79E+00 C048802400022
3.980 1.38E-07 2.09E+00 C048802400023
4.300 1.79E-07 2.09E+00 C048802400024
4.550 6.43E-07 5.97E+00 C048802400025
4.960 1.17E-06 1.19E+00 C048802400026
5.230 2.72E-06 7.47E+00 C048802400027
5.550 5.08E-06 3.59E+00 C048802400028
5.970 1.09E-05 7.47E+00 C048802400029
ENDDATA 10 0 C048802400030
ENDSUBENT 29 0 C048802499999
SUBENT C0488025 20160321 C158C048802500001
BIB 3 10 C048802500002
REACTION (50-SN-124(P,N)51-SB-124,,PY,,TT) C048802500003
ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C048802500004
. either statistical, due to number of gamma counts, C048802500005
. or set to 7% due to uncertainties in of about 5% in C048802500006
bombardment parameters such as current integration C048802500007
and 5 % in counting due to source location, etc., C048802500008
added in quadrature. C048802500009
(ERR-1) Bombardment parameters. C048802500010
(ERR-2) Source location. C048802500011
STATUS (TABLE) Table II, page 188. C048802500012
ENDBIB 10 0 C048802500013
COMMON 2 3 C048802500014
ERR-1 ERR-2 C048802500015
PER-CENT PER-CENT C048802500016
5.0 5.0 C048802500017
ENDCOMMON 3 0 C048802500018
DATA 3 9 C048802500019
EN-CM DATA DATA-ERR C048802500020
MEV PRD/INC PRD/INC C048802500021
3.983 1.19E-07 6.20E-08 C048802500022
4.305 2.68E-07 1.40E-07 C048802500023
4.550 1.10E-06 3.50E-07 C048802500024
4.686 1.33E-06 2.00E-07 C048802500025
4.961 1.37E-06 2.06E-07 C048802500026
5.122 1.84E-06 2.76E-07 C048802500027
5.233 3.07E-06 5.27E-07 C048802500028
5.550 8.25E-06 1.23E-06 C048802500029
5.967 1.09E-05 1.64E-06 C048802500030
ENDDATA 11 0 C048802500031
ENDSUBENT 30 0 C048802599999
SUBENT C0488026 20160321 C158C048802600001
BIB 3 10 C048802600002
REACTION (52-TE-123(P,N)53-I-123,,PY,,TT) C048802600003
ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C048802600004
. either statistical, due to number of gamma counts, C048802600005
. or set to 7% due to uncertainties in of about 5% in C048802600006
bombardment parameters such as current integration C048802600007
and 5 % in counting due to source location, etc., C048802600008
added in quadrature. C048802600009
(ERR-1) Bombardment parameters. C048802600010
(ERR-2) Source location. C048802600011
STATUS (TABLE) Table II, page 188. C048802600012
ENDBIB 10 0 C048802600013
COMMON 2 3 C048802600014
ERR-1 ERR-2 C048802600015
PER-CENT PER-CENT C048802600016
5.0 5.0 C048802600017
ENDCOMMON 3 0 C048802600018
DATA 3 10 C048802600019
EN-CM DATA DATA-ERR C048802600020
MEV PRD/INC PRD/INC C048802600021
3.050 1.30E-09 9.00E-10 C048802600022
3.317 1.80E-08 9.00E-10 C048802600023
3.373 1.10E-08 4.00E-10 C048802600024
3.902 2.00E-07 3.00E-08 C048802600025
4.257 3.00E-07 3.00E-08 C048802600026
4.607 1.40E-06 1.00E-08 C048802600027
5.008 3.60E-06 3.00E-07 C048802600028
5.641 9.40E-06 7.00E-07 C048802600029
6.033 1.20E-05 1.00E-07 C048802600030
6.308 1.60E-05 2.00E-06 C048802600031
ENDDATA 12 0 C048802600032
ENDSUBENT 31 0 C048802699999
SUBENT C0488027 20160321 C158C048802700001
BIB 3 10 C048802700002
REACTION (52-TE-126(P,N)53-I-126,,PY,,TT) C048802700003
ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C048802700004
. either statistical, due to number of gamma counts, C048802700005
. or set to 7% due to uncertainties in of about 5% in C048802700006
bombardment parameters such as current integration C048802700007
and 5 % in counting due to source location, etc., C048802700008
added in quadrature. C048802700009
(ERR-1) Bombardment parameters. C048802700010
(ERR-2) Source location. C048802700011
STATUS (TABLE) Table II, page 188. C048802700012
ENDBIB 10 0 C048802700013
COMMON 2 3 C048802700014
ERR-1 ERR-2 C048802700015
PER-CENT PER-CENT C048802700016
5.0 5.0 C048802700017
ENDCOMMON 3 0 C048802700018
DATA 3 10 C048802700019
EN-CM DATA DATA-ERR C048802700020
MEV PRD/INC PRD/INC C048802700021
3.005 3.40E-09 8.00E-10 C048802700022
3.320 4.50E-09 3.15E-10 C048802700023
3.374 8.10E-09 5.67E-10 C048802700024
3.903 6.20E-08 1.30E-08 C048802700025
4.258 1.10E-07 3.00E-08 C048802700026
4.608 5.30E-07 3.71E-08 C048802700027
5.009 1.60E-06 2.00E-07 C048802700028
5.642 3.80E-06 3.00E-07 C048802700029
6.034 6.30E-06 5.00E-07 C048802700030
6.310 1.10E-05 1.00E-06 C048802700031
ENDDATA 12 0 C048802700032
ENDSUBENT 31 0 C048802799999
SUBENT C0488028 20160321 C158C048802800001
BIB 3 10 C048802800002
REACTION (52-TE-128(P,N)53-I-128,,PY,,TT) C048802800003
ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C048802800004
. either statistical, due to number of gamma counts, C048802800005
. or set to 7% due to uncertainties in of about 5% in C048802800006
bombardment parameters such as current integration C048802800007
and 5 % in counting due to source location, etc., C048802800008
added in quadrature. C048802800009
(ERR-1) Bombardment parameters. C048802800010
(ERR-2) Source location. C048802800011
STATUS (TABLE) Table II, page 188. C048802800012
ENDBIB 10 0 C048802800013
COMMON 2 3 C048802800014
ERR-1 ERR-2 C048802800015
PER-CENT PER-CENT C048802800016
5.0 5.0 C048802800017
ENDCOMMON 3 0 C048802800018
DATA 3 11 C048802800019
EN-CM DATA DATA-ERR C048802800020
MEV PRD/INC PRD/INC C048802800021
2.795 5.30E-10 2.80E-10 C048802800022
3.005 7.20E-10 9.00E-11 C048802800023
3.051 6.80E-10 1.90E-10 C048802800024
3.320 4.70E-09 3.29E-10 C048802800025
3.903 4.10E-08 2.87E-09 C048802800026
4.259 9.10E-08 6.37E-09 C048802800027
4.609 3.00E-07 3.00E-08 C048802800028
5.010 7.90E-07 6.00E-08 C048802800029
5.643 2.60E-06 2.00E-07 C048802800030
6.035 5.00E-06 3.50E-07 C048802800031
6.310 5.80E-06 4.06E-07 C048802800032
ENDDATA 13 0 C048802800033
ENDSUBENT 32 0 C048802899999
SUBENT C0488029 20160321 C158C048802900001
BIB 3 10 C048802900002
REACTION (52-TE-130(P,N)53-I-130,,PY,,TT) C048802900003
ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C048802900004
. either statistical, due to number of gamma counts, C048802900005
. or set to 7% due to uncertainties in of about 5% in C048802900006
bombardment parameters such as current integration C048802900007
and 5 % in counting due to source location, etc., C048802900008
added in quadrature. C048802900009
(ERR-1) Bombardment parameters. C048802900010
(ERR-2) Source location. C048802900011
STATUS (TABLE) Table II, page 188. C048802900012
ENDBIB 10 0 C048802900013
COMMON 2 3 C048802900014
ERR-1 ERR-2 C048802900015
PER-CENT PER-CENT C048802900016
5.0 5.0 C048802900017
ENDCOMMON 3 0 C048802900018
DATA 3 12 C048802900019
EN-CM DATA DATA-ERR C048802900020
MEV PRD/INC PRD/INC C048802900021
2.796 7.00E-10 6.00E-10 C048802900022
3.006 1.80E-09 3.00E-10 C048802900023
3.052 1.10E-09 3.00E-10 C048802900024
3.321 4.90E-09 9.00E-10 C048802900025
3.375 3.40E-09 6.00E-10 C048802900026
3.904 5.50E-08 3.85E-09 C048802900027
4.259 1.10E-07 1.00E-08 C048802900028
4.610 3.80E-07 2.66E-08 C048802900029
5.011 1.10E-06 1.00E-07 C048802900030
5.644 3.60E-06 2.52E-07 C048802900031
6.036 4.90E-06 9.00E-07 C048802900032
6.312 9.50E-06 6.65E-07 C048802900033
ENDDATA 14 0 C048802900034
ENDSUBENT 33 0 C048802999999
SUBENT C0488030 20160321 C158C048803000001
BIB 3 10 C048803000002
REACTION (52-TE-130(P,N)53-I-130-M,,PY,,TT) C048803000003
ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C048803000004
. either statistical, due to number of gamma counts, C048803000005
. or set to 7% due to uncertainties in of about 5% in C048803000006
bombardment parameters such as current integration C048803000007
and 5 % in counting due to source location, etc., C048803000008
added in quadrature. C048803000009
(ERR-1) Bombardment parameters. C048803000010
(ERR-2) Source location. C048803000011
STATUS (TABLE) Table II, page 188. C048803000012
ENDBIB 10 0 C048803000013
COMMON 2 3 C048803000014
ERR-1 ERR-2 C048803000015
PER-CENT PER-CENT C048803000016
5.0 5.0 C048803000017
ENDCOMMON 3 0 C048803000018
DATA 3 8 C048803000019
EN-CM DATA DATA-ERR C048803000020
MEV PRD/INC PRD/INC C048803000021
2.796 1.30E-09 5.00E-10 C048803000022
3.052 4.90E-09 7.00E-10 C048803000023
3.321 2.30E-08 7.00E-09 C048803000024
4.259 1.80E-07 7.00E-08 C048803000025
4.610 2.10E-07 2.00E-08 C048803000026
5.011 6.80E-07 9.00E-08 C048803000027
5.644 1.70E-06 2.00E-07 C048803000028
6.312 4.40E-06 5.00E-07 C048803000029
ENDDATA 10 0 C048803000030
ENDSUBENT 29 0 C048803099999
SUBENT C0488031 20160321 C158C048803100001
BIB 3 10 C048803100002
REACTION (56-BA-134(P,N)57-LA-134,,PY,,TT) C048803100003
ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C048803100004
. either statistical, due to number of gamma counts, C048803100005
. or set to 7% due to uncertainties in of about 5% in C048803100006
bombardment parameters such as current integration C048803100007
and 5 % in counting due to source location, etc., C048803100008
added in quadrature. C048803100009
(ERR-1) Bombardment parameters. C048803100010
(ERR-2) Source location. C048803100011
STATUS (TABLE) Table II, page 188. C048803100012
ENDBIB 10 0 C048803100013
COMMON 2 3 C048803100014
ERR-1 ERR-2 C048803100015
PER-CENT PER-CENT C048803100016
5.0 5.0 C048803100017
ENDCOMMON 3 0 C048803100018
DATA 3 7 C048803100019
EN-CM DATA DATA-ERR C048803100020
MEV PRD/INC PRD/INC C048803100021
4.611 2.30E-08 6.00E-09 C048803100022
5.008 2.00E-07 2.00E-08 C048803100023
5.125 2.70E-07 2.00E-08 C048803100024
5.388 6.00E-07 5.00E-08 C048803100025
5.642 8.40E-07 8.00E-08 C048803100026
6.037 2.60E-06 3.00E-07 C048803100027
6.315 3.00E-06 3.00E-07 C048803100028
ENDDATA 9 0 C048803100029
ENDSUBENT 28 0 C048803199999
SUBENT C0488032 20160321 C158C048803200001
BIB 3 10 C048803200002
REACTION (56-BA-136(P,N)57-LA-136,,PY,,TT) C048803200003
ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C048803200004
. either statistical, due to number of gamma counts, C048803200005
. or set to 7% due to uncertainties in of about 5% in C048803200006
bombardment parameters such as current integration C048803200007
and 5 % in counting due to source location, etc., C048803200008
added in quadrature. C048803200009
(ERR-1) Bombardment parameters. C048803200010
(ERR-2) Source location. C048803200011
STATUS (TABLE) Table II, page 188. C048803200012
ENDBIB 10 0 C048803200013
COMMON 2 3 C048803200014
ERR-1 ERR-2 C048803200015
PER-CENT PER-CENT C048803200016
5.0 5.0 C048803200017
ENDCOMMON 3 0 C048803200018
DATA 3 9 C048803200019
EN-CM DATA DATA-ERR C048803200020
MEV PRD/INC PRD/INC C048803200021
3.905 5.00E-09 5.00E-09 C048803200022
4.261 5.80E-08 1.40E-08 C048803200023
4.611 9.90E-08 6.93E-09 C048803200024
5.008 2.90E-07 2.03E-08 C048803200025
5.125 4.10E-07 2.87E-08 C048803200026
5.388 7.20E-07 5.04E-08 C048803200027
5.643 1.10E-06 1.00E-07 C048803200028
6.038 3.30E-06 4.00E-07 C048803200029
6.316 3.60E-06 2.52E-07 C048803200030
ENDDATA 11 0 C048803200031
ENDSUBENT 30 0 C048803299999
SUBENT C0488033 20160321 C158C048803300001
BIB 3 10 C048803300002
REACTION (60-ND-143(P,N)61-PM-143,,PY,,TT) C048803300003
ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C048803300004
. either statistical, due to number of gamma counts, C048803300005
. or set to 7% due to uncertainties in of about 5% in C048803300006
bombardment parameters such as current integration C048803300007
and 5 % in counting due to source location, etc., C048803300008
added in quadrature. C048803300009
(ERR-1) Bombardment parameters. C048803300010
(ERR-2) Source location. C048803300011
STATUS (TABLE) Table II, page 188. C048803300012
ENDBIB 10 0 C048803300013
COMMON 2 3 C048803300014
ERR-1 ERR-2 C048803300015
PER-CENT PER-CENT C048803300016
5.0 5.0 C048803300017
ENDCOMMON 3 0 C048803300018
DATA 3 6 C048803300019
EN-CM DATA DATA-ERR C048803300020
MEV PRD/INC PRD/INC C048803300021
4.690 6.41E-08 2.14E-08 C048803300022
4.966 2.49E-07 7.11E-08 C048803300023
5.127 2.83E-07 8.90E-08 C048803300024
5.238 4.72E-07 8.90E-08 C048803300025
5.556 1.39E-06 2.09E-07 C048803300026
5.974 2.01E-06 3.02E-07 C048803300027
ENDDATA 8 0 C048803300028
ENDSUBENT 27 0 C048803399999
SUBENT C0488034 20160321 C158C048803400001
BIB 3 10 C048803400002
REACTION (60-ND-144(P,N)61-PM-144,,PY,,TT) C048803400003
ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C048803400004
. either statistical, due to number of gamma counts, C048803400005
. or set to 7% due to uncertainties in of about 5% in C048803400006
bombardment parameters such as current integration C048803400007
and 5 % in counting due to source location, etc., C048803400008
added in quadrature. C048803400009
(ERR-1) Bombardment parameters. C048803400010
(ERR-2) Source location. C048803400011
STATUS (TABLE) Table II, page 188. C048803400012
ENDBIB 10 0 C048803400013
COMMON 2 3 C048803400014
ERR-1 ERR-2 C048803400015
PER-CENT PER-CENT C048803400016
5.0 5.0 C048803400017
ENDCOMMON 3 0 C048803400018
DATA 3 7 C048803400019
EN-CM DATA DATA-ERR C048803400020
MEV PRD/INC PRD/INC C048803400021
3.850 6.20E-09 3.30E-09 C048803400022
4.690 5.23E-08 7.85E-09 C048803400023
4.967 9.20E-08 1.67E-08 C048803400024
5.128 1.51E-07 3.30E-08 C048803400025
5.238 2.05E-07 3.07E-08 C048803400026
5.556 6.32E-07 9.48E-08 C048803400027
5.974 1.46E-06 2.19E-07 C048803400028
ENDDATA 9 0 C048803400029
ENDSUBENT 28 0 C048803499999
SUBENT C0488035 20160321 C158C048803500001
BIB 3 10 C048803500002
REACTION (60-ND-146(P,N)61-PM-146,,PY,,TT) C048803500003
ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C048803500004
. either statistical, due to number of gamma counts, C048803500005
. or set to 7% due to uncertainties in of about 5% in C048803500006
bombardment parameters such as current integration C048803500007
and 5 % in counting due to source location, etc., C048803500008
added in quadrature. C048803500009
(ERR-1) Bombardment parameters. C048803500010
(ERR-2) Source location. C048803500011
STATUS (TABLE) Table II, page 188. C048803500012
ENDBIB 10 0 C048803500013
COMMON 2 3 C048803500014
ERR-1 ERR-2 C048803500015
PER-CENT PER-CENT C048803500016
5.0 5.0 C048803500017
ENDCOMMON 3 0 C048803500018
DATA 3 7 C048803500019
EN-CM DATA DATA-ERR C048803500020
MEV PRD/INC PRD/INC C048803500021
3.853 1.05E-08 9.00E-07 C048803500022
4.692 2.29E-07 1.58E-07 C048803500023
4.967 7.04E-07 6.04E-07 C048803500024
5.128 9.69E-07 3.52E-07 C048803500025
5.239 5.02E-07 3.51E-08 C048803500026
5.557 9.87E-07 2.64E-07 C048803500027
5.974 2.59E-06 3.89E-07 C048803500028
ENDDATA 9 0 C048803500029
ENDSUBENT 28 0 C048803599999
SUBENT C0488036 20160321 C158C048803600001
BIB 3 10 C048803600002
REACTION (60-ND-148(P,N)61-PM-148,,PY,,TT) C048803600003
ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C048803600004
. either statistical, due to number of gamma counts, C048803600005
. or set to 7% due to uncertainties in of about 5% in C048803600006
bombardment parameters such as current integration C048803600007
and 5 % in counting due to source location, etc., C048803600008
added in quadrature. C048803600009
(ERR-1) Bombardment parameters. C048803600010
(ERR-2) Source location. C048803600011
STATUS (TABLE) Table II, page 188. C048803600012
ENDBIB 10 0 C048803600013
COMMON 2 3 C048803600014
ERR-1 ERR-2 C048803600015
PER-CENT PER-CENT C048803600016
5.0 5.0 C048803600017
ENDCOMMON 3 0 C048803600018
DATA 3 9 C048803600019
EN-CM DATA DATA-ERR C048803600020
MEV PRD/INC PRD/INC C048803600021
3.854 5.70E-09 3.10E-09 C048803600022
4.310 7.30E-09 1.09E-09 C048803600023
4.559 3.14E-08 7.30E-09 C048803600024
4.692 5.22E-08 2.61E-08 C048803600025
4.967 7.33E-08 1.57E-08 C048803600026
5.128 1.25E-07 1.87E-08 C048803600027
5.239 2.03E-07 4.17E-08 C048803600028
5.557 3.66E-07 5.49E-08 C048803600029
5.975 7.89E-07 1.18E-07 C048803600030
ENDDATA 11 0 C048803600031
ENDSUBENT 30 0 C048803699999
SUBENT C0488037 20160321 C158C048803700001
BIB 3 10 C048803700002
REACTION (60-ND-148(P,N)61-PM-148-M,,PY,,TT) C048803700003
ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C048803700004
. either statistical, due to number of gamma counts, C048803700005
. or set to 7% due to uncertainties in of about 5% in C048803700006
bombardment parameters such as current integration C048803700007
and 5 % in counting due to source location, etc., C048803700008
added in quadrature. C048803700009
(ERR-1) Bombardment parameters. C048803700010
(ERR-2) Source location. C048803700011
STATUS (TABLE) Table II, page 188. C048803700012
ENDBIB 10 0 C048803700013
COMMON 2 3 C048803700014
ERR-1 ERR-2 C048803700015
PER-CENT PER-CENT C048803700016
5.0 5.0 C048803700017
ENDCOMMON 3 0 C048803700018
DATA 3 4 C048803700019
EN-CM DATA DATA-ERR C048803700020
MEV PRD/INC PRD/INC C048803700021
4.690 7.62E-08 3.20E-08 C048803700022
5.128 3.94E-07 5.91E-08 C048803700023
5.557 4.77E-07 7.16E-08 C048803700024
5.975 2.10E-06 3.15E-07 C048803700025
ENDDATA 6 0 C048803700026
ENDSUBENT 25 0 C048803799999
SUBENT C0488038 20160321 C158C048803800001
BIB 3 10 C048803800002
REACTION (60-ND-150(P,N)61-PM-150,,PY,,TT) C048803800003
ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C048803800004
. either statistical, due to number of gamma counts, C048803800005
. or set to 7% due to uncertainties in of about 5% in C048803800006
bombardment parameters such as current integration C048803800007
and 5 % in counting due to source location, etc., C048803800008
added in quadrature. C048803800009
(ERR-1) Bombardment parameters. C048803800010
(ERR-2) Source location. C048803800011
STATUS (TABLE) Table II, page 188. C048803800012
ENDBIB 10 0 C048803800013
COMMON 2 3 C048803800014
ERR-1 ERR-2 C048803800015
PER-CENT PER-CENT C048803800016
5.0 5.0 C048803800017
ENDCOMMON 3 0 C048803800018
DATA 3 12 C048803800019
EN-CM DATA DATA-ERR C048803800020
MEV PRD/INC PRD/INC C048803800021
2.994 9.70E-09 8.70E-09 C048803800022
3.494 6.76E-08 1.94E-08 C048803800023
3.546 1.85E-08 3.60E-09 C048803800024
3.854 7.73E-07 1.57E-07 C048803800025
3.988 8.68E-07 1.94E-07 C048803800026
4.311 3.38E-06 7.25E-07 C048803800027
4.559 4.47E-06 6.71E-07 C048803800028
4.693 5.81E-06 1.45E-06 C048803800029
4.968 9.18E-06 1.38E-06 C048803800030
5.129 1.91E-05 2.87E-06 C048803800031
5.240 1.90E-05 2.85E-06 C048803800032
5.976 1.76E-04 2.64E-05 C048803800033
ENDDATA 14 0 C048803800034
ENDSUBENT 33 0 C048803899999
SUBENT C0488039 20160321 C158C048803900001
BIB 3 10 C048803900002
REACTION (62-SM-147(P,N)63-EU-147,,PY,,TT) C048803900003
ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C048803900004
. either statistical, due to number of gamma counts, C048803900005
. or set to 7% due to uncertainties in of about 5% in C048803900006
bombardment parameters such as current integration C048803900007
and 5 % in counting due to source location, etc., C048803900008
added in quadrature. C048803900009
(ERR-1) Bombardment parameters. C048803900010
(ERR-2) Source location. C048803900011
STATUS (TABLE) Table II, page 188. C048803900012
ENDBIB 10 0 C048803900013
COMMON 2 3 C048803900014
ERR-1 ERR-2 C048803900015
PER-CENT PER-CENT C048803900016
5.0 5.0 C048803900017
ENDCOMMON 3 0 C048803900018
DATA 3 11 C048803900019
EN-CM DATA DATA-ERR C048803900020
MEV PRD/INC PRD/INC C048803900021
3.051 2.15E-09 2.15E-09 C048803900022
3.320 1.77E-10 1.80e-10 C048803900023
3.909 8.65E-09 3.60E-09 C048803900024
4.261 2.38E-08 9.00E-09 C048803900025
4.618 5.60E-08 6.50E-09 C048803900026
5.009 2.12E-07 5.00E-08 C048803900027
5.200 3.10E-07 3.60E-08 C048803900028
5.388 5.96E-07 5.40E-08 C048803900029
5.643 4.70E-07 2.20E-07 C048803900030
6.321 2.86E-06 7.20E-07 C048803900031
6.800 2.50E-06 9.00E-07 C048803900032
ENDDATA 13 0 C048803900033
ENDSUBENT 32 0 C048803999999
SUBENT C0488040 20160321 C158C048804000001
BIB 3 10 C048804000002
REACTION (62-SM-148(P,N)63-EU-148,,PY,,TT) C048804000003
ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C048804000004
. either statistical, due to number of gamma counts, C048804000005
. or set to 7% due to uncertainties in of about 5% in C048804000006
bombardment parameters such as current integration C048804000007
and 5 % in counting due to source location, etc., C048804000008
added in quadrature. C048804000009
(ERR-1) Bombardment parameters. C048804000010
(ERR-2) Source location. C048804000011
STATUS (TABLE) Table II, page 189. C048804000012
ENDBIB 10 0 C048804000013
COMMON 2 3 C048804000014
ERR-1 ERR-2 C048804000015
PER-CENT PER-CENT C048804000016
5.0 5.0 C048804000017
ENDCOMMON 3 0 C048804000018
DATA 3 9 C048804000019
EN-CM DATA DATA-ERR C048804000020
MEV PRD/INC PRD/INC C048804000021
3.905 1.80E-09 1.80E-09 C048804000022
4.260 3.60E-09 4.50E-09 C048804000023
4.610 2.66E-08 3.10E-09 C048804000024
5.009 1.46E-07 7.20E-08 C048804000025
5.199 1.67E-07 1.90E-08 C048804000026
5.390 1.93E-07 2.30E-08 C048804000027
5.650 3.70E-07 8.00E-08 C048804000028
6.312 2.25E-06 1.80E-07 C048804000029
6.799 4.32E-06 6.30E-07 C048804000030
ENDDATA 11 0 C048804000031
ENDSUBENT 30 0 C048804099999
SUBENT C0488041 20160321 C158C048804100001
BIB 3 10 C048804100002
REACTION (62-SM-149(P,N)63-EU-149,,PY,,TT) C048804100003
ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C048804100004
. either statistical, due to number of gamma counts, C048804100005
. or set to 7% due to uncertainties in of about 5% in C048804100006
bombardment parameters such as current integration C048804100007
and 5 % in counting due to source location, etc., C048804100008
added in quadrature. C048804100009
(ERR-1) Bombardment parameters. C048804100010
(ERR-2) Source location. C048804100011
STATUS (TABLE) Table II, page 189. C048804100012
ENDBIB 10 0 C048804100013
COMMON 2 3 C048804100014
ERR-1 ERR-2 C048804100015
PER-CENT PER-CENT C048804100016
5.0 5.0 C048804100017
ENDCOMMON 3 0 C048804100018
DATA 3 11 C048804100019
EN-CM DATA DATA-ERR C048804100020
MEV PRD/INC PRD/INC C048804100021
3.055 1.40E-08 1.40E-08 C048804100022
3.324 1.40E-08 4.50E-09 C048804100023
3.378 2.70E-08 9.00E-09 C048804100024
3.908 2.60E-08 1.70E-08 C048804100025
4.263 4.20E-08 1.10E-08 C048804100026
4.614 6.70E-08 1.70E-08 C048804100027
5.015 1.60E-07 8.00E-08 C048804100028
5.203 1.06E-07 6.00E-08 C048804100029
5.392 1.12E-07 6.00E-08 C048804100030
5.649 7.20E-07 5.00E-07 C048804100031
6.799 1.44E-06 4.40E-07 C048804100032
ENDDATA 13 0 C048804100033
ENDSUBENT 32 0 C048804199999
SUBENT C0488042 20160321 C158C048804200001
BIB 3 10 C048804200002
REACTION (62-SM-150(P,N)63-EU-150,,PY,,TT) C048804200003
ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C048804200004
. either statistical, due to number of gamma counts, C048804200005
. or set to 7% due to uncertainties in of about 5% in C048804200006
bombardment parameters such as current integration C048804200007
and 5 % in counting due to source location, etc., C048804200008
added in quadrature. C048804200009
(ERR-1) Bombardment parameters. C048804200010
(ERR-2) Source location. C048804200011
STATUS (TABLE) Table II, page 189. C048804200012
ENDBIB 10 0 C048804200013
COMMON 2 3 C048804200014
ERR-1 ERR-2 C048804200015
PER-CENT PER-CENT C048804200016
5.0 5.0 C048804200017
ENDCOMMON 3 0 C048804200018
DATA 3 9 C048804200019
EN-CM DATA DATA-ERR C048804200020
MEV PRD/INC PRD/INC C048804200021
3.378 3.20E-10 3.20E-10 C048804200022
4.264 1.00E-08 5.00E-09 C048804200023
4.614 4.20E-08 2.10E-08 C048804200024
5.016 8.00E-08 1.60E-08 C048804200025
5.203 1.10E-07 2.60E-08 C048804200026
5.392 1.50E-07 5.00E-08 C048804200027
5.649 3.10E-07 2.17E-08 C048804200028
6.318 1.33E-06 2.10E-07 C048804200029
6.797 3.10E-06 9.60E-07 C048804200030
ENDDATA 11 0 C048804200031
ENDSUBENT 30 0 C048804299999
SUBENT C0488043 20160321 C158C048804300001
BIB 3 10 C048804300002
REACTION (62-SM-152(P,N)63-EU-152,,PY,,TT) C048804300003
ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C048804300004
. either statistical, due to number of gamma counts, C048804300005
. or set to 7% due to uncertainties in of about 5% in C048804300006
bombardment parameters such as current integration C048804300007
and 5 % in counting due to source location, etc., C048804300008
added in quadrature. C048804300009
(ERR-1) Bombardment parameters. C048804300010
(ERR-2) Source location. C048804300011
STATUS (TABLE) Table II, page 189. C048804300012
ENDBIB 10 0 C048804300013
COMMON 2 3 C048804300014
ERR-1 ERR-2 C048804300015
PER-CENT PER-CENT C048804300016
5.0 5.0 C048804300017
ENDCOMMON 3 0 C048804300018
DATA 3 11 C048804300019
EN-CM DATA DATA-ERR C048804300020
MEV PRD/INC PRD/INC C048804300021
3.054 2.70E-10 1.80E-10 C048804300022
3.379 5.72E-10 1.95E-10 C048804300023
3.908 3.77E-09 7.00E-10 C048804300024
4.264 1.10E-08 7.70E-10 C048804300025
4.615 3.19E-08 2.23E-09 C048804300026
5.016 1.09E-07 7.63E-09 C048804300027
5.204 1.56E-07 1.09E-08 C048804300028
5.393 1.70E-07 1.40E-08 C048804300029
5.650 4.76E-07 3.33E-08 C048804300030
6.318 1.88E-06 1.32E-07 C048804300031
6.800 3.37E-06 2.36E-07 C048804300032
ENDDATA 13 0 C048804300033
ENDSUBENT 32 0 C048804399999
SUBENT C0488044 20160323 C158C048804400001
BIB 5 13 C048804400002
REACTION (5-B-10(P,A)4-BE-7,,SGV) C048804400003
ANALYSIS Thermonuclear reaction rates are usually calculated C048804400004
directly from measured reaction cross sections and C048804400005
level parameters. The relevant quantity is NA <sigma C048804400006
v>T which is Avogadro's number times the average C048804400007
value of the product of the cross section times the C048804400008
velocity, averaged over the Maxwell-Boltzmann C048804400009
velocity distribution at the temperature T of interest.C048804400010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048804400011
their values were added quadratically. C048804400012
STATUS (TABLE) Table III, page 190. C048804400013
(DEP,C0487002) C048804400014
HISTORY (20160323C) BP C048804400015
ENDBIB 13 0 C048804400016
NOCOMMON 0 0 C048804400017
DATA 3 14 C048804400018
KT DATA DATA-ERR C048804400019
K9 CM3/S/MOL CM3/S/MOL C048804400020
.500 1.90E+5 2.85E+4 C048804400021
1.000 1.44E+6 2.16E+5 C048804400022
1.500 4.64E+6 6.96E+5 C048804400023
2.000 1.10E+7 1.65E+6 C048804400024
2.500 2.08E+7 3.12E+6 C048804400025
3.000 3.30E+7 4.95E+6 C048804400026
3.500 4.64E+7 6.96E+6 C048804400027
4.000 6.01E+7 9.02E+6 C048804400028
4.500 7.32E+7 1.10E+6 C048804400029
5.000 8.52E+7 1.28E+7 C048804400030
5.500 9.60E+7 1.44E+7 C048804400031
6.000 1.05E+8 1.58E+7 C048804400032
6.500 1.13E+8 2.70E+7 C048804400033
7.000 1.20E+8 2.10E+7 C048804400034
ENDDATA 16 0 C048804400035
ENDSUBENT 34 0 C048804499999
SUBENT C0488045 20160323 C158C048804500001
BIB 5 13 C048804500002
REACTION (5-B-10(P,G)6-C-11,,SGV,,MXW) C048804500003
ANALYSIS Thermonuclear reaction rates are usually calculated C048804500004
directly from measured reaction cross sections and C048804500005
level parameters. The relevant quantity is NA <sigma C048804500006
v>T which is Avogadro's number times the average C048804500007
value of the product of the cross section times the C048804500008
velocity, averaged over the Maxwell-Boltzmann C048804500009
velocity distribution at the temperature T of interest.C048804500010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048804500011
their values were added quadratically. C048804500012
STATUS (TABLE) Table III, page 190. C048804500013
(DEP,C0487003) C048804500014
HISTORY (20160323C) BP C048804500015
ENDBIB 13 0 C048804500016
NOCOMMON 0 0 C048804500017
DATA 3 11 C048804500018
KT DATA DATA-ERR C048804500019
K9 CM3/S/MOL CM3/S/MOL C048804500020
2.000 3.93E+2 5.90E+1 C048804500021
2.500 6.50E+2 9.87E+1 C048804500022
3.000 9.62E+2 1.44E+2 C048804500023
3.500 1.28E+3 1.92E+2 C048804500024
4.000 1.60E+3 2.40E+2 C048804500025
4.500 1.91E+3 2.87E+2 C048804500026
5.000 2.21E+3 3.32E+2 C048804500027
5.500 2.40E+3 3.89E+2 C048804500028
6.000 2.72E+3 5.52E+2 C048804500029
6.500 2.93E+3 7.42E+2 C048804500030
7.000 3.12E+3 9.57E+2 C048804500031
ENDDATA 13 0 C048804500032
ENDSUBENT 31 0 C048804599999
SUBENT C0488046 20160323 C158C048804600001
BIB 5 13 C048804600002
REACTION (6-C-12(P,G)7-N-13,,SGV) C048804600003
ANALYSIS Thermonuclear reaction rates are usually calculated C048804600004
directly from measured reaction cross sections and C048804600005
level parameters. The relevant quantity is NA <sigma C048804600006
v>T which is Avogadro's number times the average C048804600007
value of the product of the cross section times the C048804600008
velocity, averaged over the Maxwell-Boltzmann C048804600009
velocity distribution at the temperature T of interest.C048804600010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048804600011
their values were added quadratically. C048804600012
STATUS (TABLE) Table III, page 190. C048804600013
(DEP,C0487004) C048804600014
HISTORY (20160323C) BP C048804600015
ENDBIB 13 0 C048804600016
NOCOMMON 0 0 C048804600017
DATA 3 13 C048804600018
KT DATA DATA-ERR C048804600019
K9 CM3/S/MOL CM3/S/MOL C048804600020
1.000 7.27E+2 1.09E+2 C048804600021
1.500 1.96E+3 2.94E+2 C048804600022
2.000 2.90E+3 4.35E+2 C048804600023
2.500 3.44E+3 5.16E+2 C048804600024
3.000 3.72E+3 5.58E+2 C048804600025
3.500 3.85E+3 5.76E+2 C048804600026
4.000 3.89E+3 5.84E+2 C048804600027
4.500 3.89E+3 5.84E+2 C048804600028
5.000 3.85E+3 5.78E+2 C048804600029
5.500 3.80E+3 5.70E+2 C048804600030
6.000 3.74E+3 5.61E+2 C048804600031
6.500 3.66E+3 5.49E+2 C048804600032
7.000 3.59E+3 6.61E+2 C048804600033
ENDDATA 15 0 C048804600034
ENDSUBENT 33 0 C048804699999
SUBENT C0488047 20160323 C158C048804700001
BIB 5 13 C048804700002
REACTION (7-N-14(P,G)8-O-15,,SGV) C048804700003
ANALYSIS Thermonuclear reaction rates are usually calculated C048804700004
directly from measured reaction cross sections and C048804700005
level parameters. The relevant quantity is NA <sigma C048804700006
v>T which is Avogadro's number times the average C048804700007
value of the product of the cross section times the C048804700008
velocity, averaged over the Maxwell-Boltzmann C048804700009
velocity distribution at the temperature T of interest.C048804700010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048804700011
their values were added quadratically. C048804700012
STATUS (TABLE) Table III, page 190. C048804700013
(DEP,C0488002) C048804700014
HISTORY (20160323C) BP C048804700015
ENDBIB 13 0 C048804700016
NOCOMMON 0 0 C048804700017
DATA 3 11 C048804700018
KT DATA DATA-ERR C048804700019
K9 CM3/S/MOL CM3/S/MOL C048804700020
1.500 4.96E+2 2.54E+2 C048804700021
2.000 6.85E+2 1.68E+2 C048804700022
2.500 9.84E+2 1.48E+2 C048804700023
3.000 1.41E+3 2.12E+2 C048804700024
3.500 1.91E+3 2.96E+2 C048804700025
4.000 2.64E+3 3.96E+2 C048804700026
4.500 3.40E+3 5.96E+2 C048804700027
5.000 4.22E+3 1.03E+3 C048804700028
5.500 5.06E+3 1.63E+3 C048804700029
6.000 5.90E+3 2.40E+3 C048804700030
6.500 6.72E+3 3.33E+3 C048804700031
ENDDATA 13 0 C048804700032
ENDSUBENT 31 0 C048804799999
SUBENT C0488048 20160323 C158C048804800001
BIB 5 13 C048804800002
REACTION (14-SI-28(P,G)15-P-29,,SGV) C048804800003
ANALYSIS Thermonuclear reaction rates are usually calculated C048804800004
directly from measured reaction cross sections and C048804800005
level parameters. The relevant quantity is NA <sigma C048804800006
v>T which is Avogadro's number times the average C048804800007
value of the product of the cross section times the C048804800008
velocity, averaged over the Maxwell-Boltzmann C048804800009
velocity distribution at the temperature T of interest.C048804800010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048804800011
their values were added quadratically. C048804800012
STATUS (TABLE) Table III, page 190. C048804800013
(DEP,C0487005) C048804800014
HISTORY (20160323C) BP C048804800015
ENDBIB 13 0 C048804800016
NOCOMMON 0 0 C048804800017
DATA 3 12 C048804800018
KT DATA DATA-ERR C048804800019
K9 CM3/S/MOL CM3/S/MOL C048804800020
1.500 2.64E+0 5.52E-1 C048804800021
2.000 2.87E+1 4.31E+0 C048804800022
2.500 1.21E+2 1.81E+1 C048804800023
3.000 3.10E+2 4.65E+1 C048804800024
3.500 5.97E+2 8.96E+1 C048804800025
4.000 9.64E+2 1.45E+2 C048804800026
4.500 1.38E+3 2.07E+2 C048804800027
5.000 1.83E+3 2.75E+2 C048804800028
5.500 2.28E+3 3.42E+2 C048804800029
6.000 2.71E+3 4.07E+2 C048804800030
6.500 3.13E+3 4.70E+2 C048804800031
7.000 3.51E+3 5.98E+2 C048804800032
ENDDATA 14 0 C048804800033
ENDSUBENT 32 0 C048804899999
SUBENT C0488049 20160323 C158C048804900001
BIB 5 13 C048804900002
REACTION (14-SI-29(P,G)15-P-30,,SGV) C048804900003
ANALYSIS Thermonuclear reaction rates are usually calculated C048804900004
directly from measured reaction cross sections and C048804900005
level parameters. The relevant quantity is NA <sigma C048804900006
v>T which is Avogadro's number times the average C048804900007
value of the product of the cross section times the C048804900008
velocity, averaged over the Maxwell-Boltzmann C048804900009
velocity distribution at the temperature T of interest.C048804900010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048804900011
their values were added quadratically. C048804900012
STATUS (TABLE) Table III, page 190. C048804900013
(DEP,C0487006) C048804900014
HISTORY (20160323C) BP C048804900015
ENDBIB 13 0 C048804900016
NOCOMMON 0 0 C048804900017
DATA 3 10 C048804900018
KT DATA DATA-ERR C048804900019
K9 CM3/S/MOL CM3/S/MOL C048804900020
2.000 2.84E+3 7.78E+2 C048804900021
2.500 3.55E+3 5.47E+2 C048804900022
3.000 4.40E+3 6.60E+2 C048804900023
3.500 5.48E+3 8.22E+2 C048804900024
4.000 6.81E+3 1.02E+3 C048804900025
4.500 8.35E+3 1.25E+3 C048804900026
5.000 1.01E+4 1.52E+3 C048804900027
5.500 1.19E+4 1.79E+3 C048804900028
6.000 1.37E+4 2.06E+3 C048804900029
6.500 1.55E+4 2.33E+3 C048804900030
ENDDATA 12 0 C048804900031
ENDSUBENT 30 0 C048804999999
SUBENT C0488050 20160323 C158C048805000001
BIB 5 13 C048805000002
REACTION (20-CA-40(P,G)21-SC-41,,SGV) C048805000003
ANALYSIS Thermonuclear reaction rates are usually calculated C048805000004
directly from measured reaction cross sections and C048805000005
level parameters. The relevant quantity is NA <sigma C048805000006
v>T which is Avogadro's number times the average C048805000007
value of the product of the cross section times the C048805000008
velocity, averaged over the Maxwell-Boltzmann C048805000009
velocity distribution at the temperature T of interest.C048805000010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048805000011
their values were added quadratically. C048805000012
STATUS (TABLE) Table III, page 190. C048805000013
(DEP,C0487007) C048805000014
HISTORY (20160323C) BP C048805000015
ENDBIB 13 0 C048805000016
NOCOMMON 0 0 C048805000017
DATA 3 10 C048805000018
KT DATA DATA-ERR C048805000019
K9 CM3/S/MOL CM3/S/MOL C048805000020
3.500 3.25E+1 9.62E+0 C048805000021
4.000 4.51E+1 8.77E+0 C048805000022
4.500 6.17E+1 9.25E+0 C048805000023
5.000 8.28E+1 1.24E+1 C048805000024
5.500 1.09E+2 1.64E+1 C048805000025
6.000 1.40E+2 2.10E+1 C048805000026
6.500 1.77E+2 2.66E+1 C048805000027
7.000 2.17E+2 3.25E+1 C048805000028
7.500 2.62E+2 3.93E+1 C048805000029
8.000 3.11E+2 5.55E+1 C048805000030
ENDDATA 12 0 C048805000031
ENDSUBENT 30 0 C048805099999
SUBENT C0488051 20160323 C158C048805100001
BIB 5 13 C048805100002
REACTION (22-TI-46(P,G)23-V-47,,SGV) C048805100003
ANALYSIS Thermonuclear reaction rates are usually calculated C048805100004
directly from measured reaction cross sections and C048805100005
level parameters. The relevant quantity is NA <sigma C048805100006
v>T which is Avogadro's number times the average C048805100007
value of the product of the cross section times the C048805100008
velocity, averaged over the Maxwell-Boltzmann C048805100009
velocity distribution at the temperature T of interest.C048805100010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048805100011
their values were added quadratically. C048805100012
STATUS (TABLE) Table III, page 190. C048805100013
(DEP,C0487008) C048805100014
HISTORY (20160323C) BP C048805100015
ENDBIB 13 0 C048805100016
NOCOMMON 0 0 C048805100017
DATA 3 12 C048805100018
KT DATA DATA-ERR C048805100019
K9 CM3/S/MOL CM3/S/MOL C048805100020
1.500 2.16E+2 3.24E+1 C048805100021
2.000 9.49E+2 1.42E+2 C048805100022
2.500 2.50E+3 3.75E+2 C048805100023
3.000 4.98E+3 7.47E+2 C048805100024
3.500 8.35E+3 1.25E+3 C048805100025
4.000 1.25E+4 1.88E+3 C048805100026
4.500 1.72E+4 2.58E+3 C048805100027
5.000 2.23E+4 3.35E+3 C048805100028
5.500 2.77E+4 4.16E+3 C048805100029
6.000 3.31E+4 4.97E+3 C048805100030
6.500 3.85E+4 5.97E+3 C048805100031
7.000 4.37E+4 8.48E+3 C048805100032
ENDDATA 14 0 C048805100033
ENDSUBENT 32 0 C048805199999
SUBENT C0488052 20160323 C158C048805200001
BIB 5 13 C048805200002
REACTION (22-TI-47(P,G)23-V-48,,SGV) C048805200003
ANALYSIS Thermonuclear reaction rates are usually calculated C048805200004
directly from measured reaction cross sections and C048805200005
level parameters. The relevant quantity is NA <sigma C048805200006
v>T which is Avogadro's number times the average C048805200007
value of the product of the cross section times the C048805200008
velocity, averaged over the Maxwell-Boltzmann C048805200009
velocity distribution at the temperature T of interest.C048805200010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048805200011
their values were added quadratically. C048805200012
STATUS (TABLE) Table III, page 190. C048805200013
(DEP,C0487009) C048805200014
HISTORY (20160323C) BP C048805200015
ENDBIB 13 0 C048805200016
NOCOMMON 0 0 C048805200017
DATA 3 12 C048805200018
KT DATA DATA-ERR C048805200019
K9 CM3/S/MOL CM3/S/MOL C048805200020
1.500 3.47E+2 6.18E+1 C048805200021
2.000 1.83E+3 2.75E+2 C048805200022
2.500 5.42E+3 8.13E+2 C048805200023
3.000 1.17E+4 1.76E+3 C048805200024
3.500 2.09E+4 3.14E+3 C048805200025
4.000 3.29E+4 4.94E+3 C048805200026
4.500 4.72E+4 7.08E+3 C048805200027
5.000 6.36E+4 9.54E+3 C048805200028
5.500 8.14E+4 1.22E+4 C048805200029
6.000 1.00E+5 1.50E+4 C048805200030
6.500 1.20E+5 1.80E+4 C048805200031
7.000 1.39E+5 2.09E+4 C048805200032
ENDDATA 14 0 C048805200033
ENDSUBENT 32 0 C048805299999
SUBENT C0488053 20160323 C158C048805300001
BIB 5 13 C048805300002
REACTION (24-CR-50(P,G)25-MN-51,,SGV) C048805300003
ANALYSIS Thermonuclear reaction rates are usually calculated C048805300004
directly from measured reaction cross sections and C048805300005
level parameters. The relevant quantity is NA <sigma C048805300006
v>T which is Avogadro's number times the average C048805300007
value of the product of the cross section times the C048805300008
velocity, averaged over the Maxwell-Boltzmann C048805300009
velocity distribution at the temperature T of interest.C048805300010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048805300011
their values were added quadratically. C048805300012
STATUS (TABLE) Table III, page 190. C048805300013
(DEP,C0487010) C048805300014
HISTORY (20160323C) BP C048805300015
ENDBIB 13 0 C048805300016
NOCOMMON 0 0 C048805300017
DATA 3 13 C048805300018
KT DATA DATA-ERR C048805300019
K9 CM3/S/MOL CM3/S/MOL C048805300020
1.000 1.99E+0 4.22E-1 C048805300021
1.500 5.45E+1 8.18E+0 C048805300022
2.000 2.98E+2 4.47E+1 C048805300023
2.500 8.74E+2 1.31E+2 C048805300024
3.000 1.58E+3 2.82E+2 C048805300025
3.000 3.36E+3 5.04E+2 C048805300026
4.000 5.31E+3 7.97E+2 C048805300027
4.500 7.72E+3 1.16E+3 C048805300028
5.000 1.05E+4 1.58E+3 C048805300029
5.500 1.37E+4 2.06E+3 C048805300030
6.000 1.72E+4 2.58E+3 C048805300031
6.500 2.09E+4 3.14E+3 C048805300032
7.000 2.48E+4 3.72E+3 C048805300033
ENDDATA 15 0 C048805300034
ENDSUBENT 33 0 C048805399999
SUBENT C0488054 20160323 C158C048805400001
BIB 5 13 C048805400002
REACTION (26-FE-54(P,G)27-CO-55,,SGV) C048805400003
ANALYSIS Thermonuclear reaction rates are usually calculated C048805400004
directly from measured reaction cross sections and C048805400005
level parameters. The relevant quantity is NA <sigma C048805400006
v>T which is Avogadro's number times the average C048805400007
value of the product of the cross section times the C048805400008
velocity, averaged over the Maxwell-Boltzmann C048805400009
velocity distribution at the temperature T of interest.C048805400010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048805400011
their values were added quadratically. C048805400012
STATUS (TABLE) Table III, page 190. C048805400013
(DEP,C0487011) C048805400014
HISTORY (20160323C) BP C048805400015
ENDBIB 13 0 C048805400016
NOCOMMON 0 0 C048805400017
DATA 3 10 C048805400018
KT DATA DATA-ERR C048805400019
K9 CM3/S/MOL CM3/S/MOL C048805400020
2.500 2.78E+2 7.28E+1 C048805400021
3.000 5.28E+2 7.92E+1 C048805400022
3.500 9.16E+2 1.37E+2 C048805400023
4.000 1.46E+3 2.19E+2 C048805400024
4.500 2.16E+3 3.24E+2 C048805400025
5.000 2.99E+3 4.49E+2 C048805400026
5.500 3.94E+3 5.91E+2 C048805400027
6.000 4.96E+3 8.44E+2 C048805400028
6.500 6.02E+3 1.27E+3 C048805400029
7.000 7.10E+3 1.81E+3 C048805400030
ENDDATA 12 0 C048805400031
ENDSUBENT 30 0 C048805499999
SUBENT C0488055 20160323 C158C048805500001
BIB 5 13 C048805500002
REACTION (26-FE-56(P,G)27-CO-57,,SGV) C048805500003
ANALYSIS Thermonuclear reaction rates are usually calculated C048805500004
directly from measured reaction cross sections and C048805500005
level parameters. The relevant quantity is NA <sigma C048805500006
v>T which is Avogadro's number times the average C048805500007
value of the product of the cross section times the C048805500008
velocity, averaged over the Maxwell-Boltzmann C048805500009
velocity distribution at the temperature T of interest.C048805500010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048805500011
their values were added quadratically. C048805500012
STATUS (TABLE) Table III, page 190. C048805500013
(DEP,C0487012) C048805500014
HISTORY (20160323C) BP C048805500015
ENDBIB 13 0 C048805500016
NOCOMMON 0 0 C048805500017
DATA 3 5 C048805500018
KT DATA DATA-ERR C048805500019
K9 CM3/S/MOL CM3/S/MOL C048805500020
1.500 8.86E+1 4.98E+1 C048805500021
2.000 3.57E+2 1.11E+2 C048805500022
2.500 8.62E+2 2.85E+2 C048805500023
3.000 1.55E+3 6.98E+2 C048805500024
3.500 2.33E+3 1.39E+3 C048805500025
ENDDATA 7 0 C048805500026
ENDSUBENT 25 0 C048805599999
SUBENT C0488056 20160323 C158C048805600001
BIB 5 13 C048805600002
REACTION (28-NI-58(P,G)29-CU-59,,SGV) C048805600003
ANALYSIS Thermonuclear reaction rates are usually calculated C048805600004
directly from measured reaction cross sections and C048805600005
level parameters. The relevant quantity is NA <sigma C048805600006
v>T which is Avogadro's number times the average C048805600007
value of the product of the cross section times the C048805600008
velocity, averaged over the Maxwell-Boltzmann C048805600009
velocity distribution at the temperature T of interest.C048805600010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048805600011
their values were added quadratically. C048805600012
STATUS (TABLE) Table III, page 190. C048805600013
(DEP,C0487013) C048805600014
HISTORY (20160323C) BP C048805600015
ENDBIB 13 0 C048805600016
NOCOMMON 0 0 C048805600017
DATA 3 8 C048805600018
KT DATA DATA-ERR C048805600019
K9 CM3/S/MOL CM3/S/MOL C048805600020
2.500 1.03E+2 3.00E+1 C048805600021
3.000 2.45E+2 4.62E+1 C048805600022
3.500 4.71E+2 7.07E+1 C048805600023
4.000 7.92E+2 1.19E+2 C048805600024
4.500 1.21E+3 1.82E+2 C048805600025
5.000 1.73E+3 3.05E+2 C048805600026
5.500 2.34E+3 5.67E+2 C048805600027
6.000 3.02E+3 4.53E+2 C048805600028
ENDDATA 10 0 C048805600029
ENDSUBENT 28 0 C048805699999
SUBENT C0488057 20160323 C158C048805700001
BIB 5 13 C048805700002
REACTION (28-NI-60(P,G)29-CU-61,,SGV) C048805700003
ANALYSIS Thermonuclear reaction rates are usually calculated C048805700004
directly from measured reaction cross sections and C048805700005
level parameters. The relevant quantity is NA <sigma C048805700006
v>T which is Avogadro's number times the average C048805700007
value of the product of the cross section times the C048805700008
velocity, averaged over the Maxwell-Boltzmann C048805700009
velocity distribution at the temperature T of interest.C048805700010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048805700011
their values were added quadratically. C048805700012
STATUS (TABLE) Table III, page 190. C048805700013
(DEP,C0487014) C048805700014
HISTORY (20160323C) BP C048805700015
ENDBIB 13 0 C048805700016
NOCOMMON 0 0 C048805700017
DATA 3 12 C048805700018
KT DATA DATA-ERR C048805700019
K9 CM3/S/MOL CM3/S/MOL C048805700020
1.500 1.28E+1 1.92E+0 C048805700021
2.000 1.16E+2 1.74E+1 C048805700022
2.500 4.93E+2 7.40E+1 C048805700023
3.000 1.35E+3 2.03E+2 C048805700024
3.500 2.83E+3 4.25E+2 C048805700025
4.000 4.95E+3 7.43E+2 C048805700026
4.500 7.64E+3 1.15E+3 C048805700027
5.000 1.08E+4 2.02E+3 C048805700028
5.500 1.42E+4 3.42E+3 C048805700029
6.000 1.78E+4 5.32E+3 C048805700030
6.500 2.14E+4 7.70E+3 C048805700031
7.000 2.49E+4 1.05E+4 C048805700032
ENDDATA 14 0 C048805700033
ENDSUBENT 32 0 C048805799999
SUBENT C0488058 20160323 C158C048805800001
BIB 5 13 C048805800002
REACTION (28-NI-61(P,G)29-CU-62,,SGV) C048805800003
ANALYSIS Thermonuclear reaction rates are usually calculated C048805800004
directly from measured reaction cross sections and C048805800005
level parameters. The relevant quantity is NA <sigma C048805800006
v>T which is Avogadro's number times the average C048805800007
value of the product of the cross section times the C048805800008
velocity, averaged over the Maxwell-Boltzmann C048805800009
velocity distribution at the temperature T of interest.C048805800010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048805800011
their values were added quadratically. C048805800012
STATUS (TABLE) Table III, page 190. C048805800013
(DEP,C0487015) C048805800014
HISTORY (20160323C) BP C048805800015
ENDBIB 13 0 C048805800016
NOCOMMON 0 0 C048805800017
DATA 3 12 C048805800018
KT DATA DATA-ERR C048805800019
K9 CM3/S/MOL CM3/S/MOL C048805800020
1.500 3.21E+1 4.81E+0 C048805800021
2.000 3.17E+2 4.76E+1 C048805800022
2.500 1.38E+3 2.07E+2 C048805800023
3.000 3.93E+3 5.90E+2 C048805800024
3.500 8.71E+3 1.31E+3 C048805800025
4.000 1.62E+4 2.43E+3 C048805800026
4.500 2.66E+4 3.99E+3 C048805800027
5.000 3.97E+4 5.96E+3 C048805800028
5.500 5.52E+4 9.33E+3 C048805800029
6.000 7.25E+4 1.57E+4 C048805800030
6.500 9.11E+4 2.44E+4 C048805800031
7.000 1.10E+5 3.53E+4 C048805800032
ENDDATA 14 0 C048805800033
ENDSUBENT 32 0 C048805899999
SUBENT C0488059 20160323 C158C048805900001
BIB 5 13 C048805900002
REACTION (30-ZN-64(P,G)31-GA-65,,SGV) C048805900003
ANALYSIS Thermonuclear reaction rates are usually calculated C048805900004
directly from measured reaction cross sections and C048805900005
level parameters. The relevant quantity is NA <sigma C048805900006
v>T which is Avogadro's number times the average C048805900007
value of the product of the cross section times the C048805900008
velocity, averaged over the Maxwell-Boltzmann C048805900009
velocity distribution at the temperature T of interest.C048805900010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048805900011
their values were added quadratically. C048805900012
STATUS (TABLE) Table III, page 191. C048805900013
(DEP,C0487016) C048805900014
HISTORY (20160323C) BP C048805900015
ENDBIB 13 0 C048805900016
NOCOMMON 0 0 C048805900017
DATA 3 13 C048805900018
KT DATA DATA-ERR C048805900019
K9 CM3/S/MOL CM3/S/MOL C048805900020
1.000 8.11E-2 1.22E-2 C048805900021
1.500 5.31E+0 7.97E-1 C048805900022
2.000 6.00E+1 9.00E+0 C048805900023
2.500 2.97E+2 4.46E+1 C048805900024
3.000 9.31E+2 1.40E+2 C048805900025
3.500 2.20E+3 3.30E+2 C048805900026
4.000 4.32E+3 6.48E+2 C048805900027
4.500 7.44E+3 1.12E+3 C048805900028
5.000 1.16E+4 1.74E+3 C048805900029
5.500 1.69E+4 2.54E+3 C048805900030
6.000 2.33E+4 3.50E+3 C048805900031
6.500 3.05E+4 4.58E+3 C048805900032
7.000 3.86E+4 5.79E+3 C048805900033
ENDDATA 15 0 C048805900034
ENDSUBENT 33 0 C048805999999
SUBENT C0488060 20160323 C158C048806000001
BIB 5 13 C048806000002
REACTION (30-ZN-67(P,G)31-GA-68,,SGV) C048806000003
ANALYSIS Thermonuclear reaction rates are usually calculated C048806000004
directly from measured reaction cross sections and C048806000005
level parameters. The relevant quantity is NA <sigma C048806000006
v>T which is Avogadro's number times the average C048806000007
value of the product of the cross section times the C048806000008
velocity, averaged over the Maxwell-Boltzmann C048806000009
velocity distribution at the temperature T of interest.C048806000010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048806000011
their values were added quadratically. C048806000012
STATUS (TABLE) Table III, page 191. C048806000013
(DEP,C0487017) C048806000014
HISTORY (20160323C) BP C048806000015
ENDBIB 13 0 C048806000016
NOCOMMON 0 0 C048806000017
DATA 3 13 C048806000018
KT DATA DATA-ERR C048806000019
K9 CM3/S/MOL CM3/S/MOL C048806000020
1.000 2.52E-1 3.78E-2 C048806000021
1.500 2.15E+1 3.23E+0 C048806000022
2.000 2.53E+2 3.80E+1 C048806000023
2.500 1.22E+3 1.83E+2 C048806000024
3.000 3.64E+3 5.46E+2 C048806000025
3.500 8.11E+3 1.22E+3 C048806000026
4.000 1.50E+4 2.25E+3 C048806000027
4.500 2.43E+4 3.65E+3 C048806000028
5.000 3.58E+4 5.37E+3 C048806000029
5.500 4.91E+4 7.37E+3 C048806000030
6.000 6.38E+4 9.57E+3 C048806000031
6.500 7.95E+4 1.41E+4 C048806000032
7.000 9.57E+4 2.08E+4 C048806000033
ENDDATA 15 0 C048806000034
ENDSUBENT 33 0 C048806099999
SUBENT C0488061 20160323 C158C048806100001
BIB 5 13 C048806100002
REACTION (32-GE-70(P,G)33-AS-71,,SGV) C048806100003
ANALYSIS Thermonuclear reaction rates are usually calculated C048806100004
directly from measured reaction cross sections and C048806100005
level parameters. The relevant quantity is NA <sigma C048806100006
v>T which is Avogadro's number times the average C048806100007
value of the product of the cross section times the C048806100008
velocity, averaged over the Maxwell-Boltzmann C048806100009
velocity distribution at the temperature T of interest.C048806100010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048806100011
their values were added quadratically. C048806100012
STATUS (TABLE) Table III, page 191. C048806100013
(DEP,C0487018) C048806100014
HISTORY (20160323C) BP C048806100015
ENDBIB 13 0 C048806100016
NOCOMMON 0 0 C048806100017
DATA 3 11 C048806100018
KT DATA DATA-ERR C048806100019
K9 CM3/S/MOL CM3/S/MOL C048806100020
2.000 5.59E+1 1.60E+1 C048806100021
2.500 3.58E+2 5.37E+1 C048806100022
3.000 1.38E+3 2.07E+2 C048806100023
3.800 3.92E+3 5.88E+2 C048806100024
4.000 8.98E+3 1.35E+3 C048806100025
4.500 1.77E+4 2.66E+3 C048806100026
5.000 3.10E+4 4.65E+3 C048806100027
5.500 4.99E+4 7.49E+3 C048806100028
6.000 7.47E+4 1.12E+4 C048806100029
6.500 1.06E+5 1.59E+4 C048806100030
7.000 1.43E+5 2.35E+4 C048806100031
ENDDATA 13 0 C048806100032
ENDSUBENT 31 0 C048806199999
SUBENT C0488062 20160323 C158C048806200001
BIB 5 13 C048806200002
REACTION (38-SR-87(P,G)39-Y-88,,SGV) C048806200003
ANALYSIS Thermonuclear reaction rates are usually calculated C048806200004
directly from measured reaction cross sections and C048806200005
level parameters. The relevant quantity is NA <sigma C048806200006
v>T which is Avogadro's number times the average C048806200007
value of the product of the cross section times the C048806200008
velocity, averaged over the Maxwell-Boltzmann C048806200009
velocity distribution at the temperature T of interest.C048806200010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048806200011
their values were added quadratically. C048806200012
STATUS (TABLE) Table III, page 191. C048806200013
(DEP,C0488003) C048806200014
HISTORY (20160323C) BP C048806200015
ENDBIB 13 0 C048806200016
NOCOMMON 0 0 C048806200017
DATA 3 9 C048806200018
KT DATA DATA-ERR C048806200019
K9 CM3/S/MOL CM3/S/MOL C048806200020
5.000 5.59E+5 1.78E+5 C048806200021
5.500 8.65E+5 2.02E+5 C048806200022
6.000 1.25E+6 2.36E+5 C048806200023
6.500 1.71E+6 2.94E+5 C048806200024
7.000 2.23E+6 3.87E+5 C048806200025
7.500 2.81E+6 5.37E+5 C048806200026
8.000 3.44E+6 7.61E+5 C048806200027
8.500 4.10E+6 1.13E+6 C048806200028
9.000 4.79E+6 1.51E+6 C048806200029
ENDDATA 11 0 C048806200030
ENDSUBENT 29 0 C048806299999
SUBENT C0488063 20160323 C158C048806300001
BIB 5 13 C048806300002
REACTION (40-ZR-90(P,G)41-NB-91-M,,SGV) C048806300003
ANALYSIS Thermonuclear reaction rates are usually calculated C048806300004
directly from measured reaction cross sections and C048806300005
level parameters. The relevant quantity is NA <sigma C048806300006
v>T which is Avogadro's number times the average C048806300007
value of the product of the cross section times the C048806300008
velocity, averaged over the Maxwell-Boltzmann C048806300009
velocity distribution at the temperature T of interest.C048806300010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048806300011
their values were added quadratically. C048806300012
STATUS (TABLE) Table III, page 191. C048806300013
(DEP,C0488004) C048806300014
HISTORY (20160323C) BP C048806300015
ENDBIB 13 0 C048806300016
NOCOMMON 0 0 C048806300017
DATA 3 12 C048806300018
KT DATA DATA-ERR C048806300019
K9 CM3/S/MOL CM3/S/MOL C048806300020
2.500 7.27E+1 4.15E+1 C048806300021
3.000 2.76E+2 8.36E+1 C048806300022
3.500 8.15E+2 1.33E+2 C048806300023
4.000 2.04E+3 3.06E+2 C048806300024
4.500 4.53E+3 6.80E+2 C048806300025
5.000 9.08E+3 1.36E+3 C048806300026
5.500 1.61E+4 2.51E+3 C048806300027
6.000 2.86E+4 4.29E+3 C048806300028
6.500 4.60E+4 8.90E+3 C048806300029
7.000 7.00E+4 1.05E+4 C048806300030
7.500 1.01E+5 1.52E+4 C048806300031
8.000 1.41E+5 2.45E+4 C048806300032
ENDDATA 14 0 C048806300033
ENDSUBENT 32 0 C048806399999
SUBENT C0488064 20160323 C158C048806400001
BIB 5 13 C048806400002
REACTION (42-MO-92(P,G)43-TC-93,,SGV) C048806400003
ANALYSIS Thermonuclear reaction rates are usually calculated C048806400004
directly from measured reaction cross sections and C048806400005
level parameters. The relevant quantity is NA <sigma C048806400006
v>T which is Avogadro's number times the average C048806400007
value of the product of the cross section times the C048806400008
velocity, averaged over the Maxwell-Boltzmann C048806400009
velocity distribution at the temperature T of interest.C048806400010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048806400011
their values were added quadratically. C048806400012
STATUS (TABLE) Table III, page 191. C048806400013
(DEP,C0487019) C048806400014
HISTORY (20160323C) BP C048806400015
ENDBIB 13 0 C048806400016
NOCOMMON 0 0 C048806400017
DATA 3 11 C048806400018
KT DATA DATA-ERR C048806400019
K9 CM3/S/MOL CM3/S/MOL C048806400020
2.000 1.45E+0 4.94E-1 C048806400021
2.500 1.05E+1 1.58E+0 C048806400022
3.000 4.65E+1 6.98E+0 C048806400023
3.500 1.51E+2 2.27E+1 C048806400024
4.000 3.92E+2 5.88E+1 C048806400025
4.500 8.65E+2 1.30E+2 C048806400026
5.000 1.67E+3 2.51E+2 C048806400027
5.500 2.92E+3 4.38E+2 C048806400028
6.000 4.69E+3 8.42E+2 C048806400029
6.500 7.03E+3 1.62E+3 C048806400030
7.000 9.96E+3 2.81E+3 C048806400031
ENDDATA 13 0 C048806400032
ENDSUBENT 31 0 C048806499999
SUBENT C0488065 20160323 C158C048806500001
BIB 5 13 C048806500002
REACTION (42-MO-92(P,G)43-TC-93-M,,SGV) C048806500003
ANALYSIS Thermonuclear reaction rates are usually calculated C048806500004
directly from measured reaction cross sections and C048806500005
level parameters. The relevant quantity is NA <sigma C048806500006
v>T which is Avogadro's number times the average C048806500007
value of the product of the cross section times the C048806500008
velocity, averaged over the Maxwell-Boltzmann C048806500009
velocity distribution at the temperature T of interest.C048806500010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048806500011
their values were added quadratically. C048806500012
STATUS (TABLE) Table III, page 191. C048806500013
(DEP,C0487020) C048806500014
HISTORY (20160323C) BP C048806500015
ENDBIB 13 0 C048806500016
NOCOMMON 0 0 C048806500017
DATA 3 11 C048806500018
KT DATA DATA-ERR C048806500019
K9 CM3/S/MOL CM3/S/MOL C048806500020
2.000 6.21E-1 1.82E-1 C048806500021
2.500 4.50E+0 6.75E-1 C048806500022
3.000 1.95E+1 2.93E+0 C048806500023
3.500 6.14E+1 9.21E+0 C048806500024
4.000 1.55E+2 2.33E+1 C048806500025
4.500 3.36E+2 5.04E+1 C048806500026
5.000 6.40E+2 9.60E+1 C048806500027
5.500 1.11E+3 1.67E+2 C048806500028
6.000 1.77E+3 3.23E+2 C048806500029
6.500 2.64E+3 6.22E+2 C048806500030
7.000 3.74E+3 1.10E+3 C048806500031
ENDDATA 13 0 C048806500032
ENDSUBENT 31 0 C048806599999
SUBENT C0488066 20160323 C158C048806600001
BIB 5 13 C048806600002
REACTION (42-MO-95(P,G)43-TC-96,,SGV) C048806600003
ANALYSIS Thermonuclear reaction rates are usually calculated C048806600004
directly from measured reaction cross sections and C048806600005
level parameters. The relevant quantity is NA <sigma C048806600006
v>T which is Avogadro's number times the average C048806600007
value of the product of the cross section times the C048806600008
velocity, averaged over the Maxwell-Boltzmann C048806600009
velocity distribution at the temperature T of interest.C048806600010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048806600011
their values were added quadratically. C048806600012
STATUS (TABLE) Table III, page 191. C048806600013
(DEP,C0487021) C048806600014
HISTORY (20160323C) BP C048806600015
ENDBIB 13 0 C048806600016
NOCOMMON 0 0 C048806600017
DATA 3 10 C048806600018
KT DATA DATA-ERR C048806600019
K9 CM3/S/MOL CM3/S/MOL C048806600020
2.500 4.42E+1 9.28E+0 C048806600021
3.000 1.90E+2 2.85E+1 C048806600022
3.500 5.65E+2 8.48E+1 C048806600023
4.000 1.31E+3 1.97E+2 C048806600024
4.500 2.56E+3 3.84E+2 C048806600025
5.000 4.39E+3 6.59E+2 C048806600026
5.500 6.86E+3 1.03E+3 C048806600027
6.000 9.96E+3 1.49E+3 C048806600028
6.500 1.36E+4 2.04E+3 C048806600029
7.000 1.78E+4 3.32E+3 C048806600030
ENDDATA 12 0 C048806600031
ENDSUBENT 30 0 C048806699999
SUBENT C0488067 20160323 C158C048806700001
BIB 5 13 C048806700002
REACTION (42-MO-95(P,G)43-TC-96-M,,SGV) C048806700003
ANALYSIS Thermonuclear reaction rates are usually calculated C048806700004
directly from measured reaction cross sections and C048806700005
level parameters. The relevant quantity is NA <sigma C048806700006
v>T which is Avogadro's number times the average C048806700007
value of the product of the cross section times the C048806700008
velocity, averaged over the Maxwell-Boltzmann C048806700009
velocity distribution at the temperature T of interest.C048806700010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048806700011
their values were added quadratically. C048806700012
STATUS (TABLE) Table III, page 191. C048806700013
(DEP,C0487022) C048806700014
HISTORY (20160323C) BP C048806700015
ENDBIB 13 0 C048806700016
NOCOMMON 0 0 C048806700017
DATA 3 10 C048806700018
KT DATA DATA-ERR C048806700019
K9 CM3/S/MOL CM3/S/MOL C048806700020
2.500 1.75E+0 1.24E+0 C048806700021
3.000 7.97E+0 3.70E+0 C048806700022
3.500 2.35E+1 8.45E+0 C048806700023
4.000 5.29E+1 1.69E+1 C048806700024
4.500 9.87E+1 3.21E+1 C048806700025
5.000 1.62E+2 5.84E+1 C048806700026
5.800 2.40E+2 9.93E+1 C048806700027
6.000 3.32E+2 9.45E+1 C048806700028
6.500 4.34E+2 2.38E+2 C048806700029
7.000 5.42E+2 3.25E+2 C048806700030
ENDDATA 12 0 C048806700031
ENDSUBENT 30 0 C048806799999
SUBENT C0488068 20160323 C158C048806800001
BIB 5 13 C048806800002
REACTION (42-MO-98(P,G)43-TC-99-M,,SGV) C048806800003
ANALYSIS Thermonuclear reaction rates are usually calculated C048806800004
directly from measured reaction cross sections and C048806800005
level parameters. The relevant quantity is NA <sigma C048806800006
v>T which is Avogadro's number times the average C048806800007
value of the product of the cross section times the C048806800008
velocity, averaged over the Maxwell-Boltzmann C048806800009
velocity distribution at the temperature T of interest.C048806800010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048806800011
their values were added quadratically. C048806800012
STATUS (TABLE) Table III, page 191. C048806800013
(DEP,C0487023) C048806800014
HISTORY (20160323C) BP C048806800015
ENDBIB 13 0 C048806800016
NOCOMMON 0 0 C048806800017
DATA 3 8 C048806800018
KT DATA DATA-ERR C048806800019
K9 CM3/S/MOL CM3/S/MOL C048806800020
1.500 1.85E+0 4.72E-1 C048806800021
2.000 5.47E+1 8.20E+0 C048806800022
2.500 4.68E+2 7.02E+1 C048806800023
3.000 2.02E+3 3.03E+2 C048806800024
3.500 5.82E+3 8.73E+2 C048806800025
4.000 1.29E+4 1.94E+3 C048806800026
4.500 2.36E+4 3.57E+3 C048806800027
5.000 3.90E+4 5.85E+3 C048806800028
ENDDATA 10 0 C048806800029
ENDSUBENT 28 0 C048806899999
SUBENT C0488069 20160323 C158C048806900001
BIB 5 13 C048806900002
REACTION (42-MO-100(P,G)43-TC-101,,SGV) C048806900003
ANALYSIS Thermonuclear reaction rates are usually calculated C048806900004
directly from measured reaction cross sections and C048806900005
level parameters. The relevant quantity is NA <sigma C048806900006
v>T which is Avogadro's number times the average C048806900007
value of the product of the cross section times the C048806900008
velocity, averaged over the Maxwell-Boltzmann C048806900009
velocity distribution at the temperature T of interest.C048806900010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048806900011
their values were added quadratically. C048806900012
STATUS (TABLE) Table III, page 191. C048806900013
(DEP,C0487024) C048806900014
HISTORY (20160323C) BP C048806900015
ENDBIB 13 0 C048806900016
NOCOMMON 0 0 C048806900017
DATA 3 10 C048806900018
KT DATA DATA-ERR C048806900019
K9 CM3/S/MOL CM3/S/MOL C048806900020
2.500 3.64E-1 1.22E-1 C048806900021
3.000 1.86E+0 3.05E-1 C048806900022
3.500 6.83E+0 1.02E+0 C048806900023
4.000 1.99E+1 2.98E+0 C048806900024
4.500 4.80E+1 7.20E+0 C048806900025
5.000 1.00E+2 1.50E+1 C048806900026
5.500 1.85E+2 3.79E+1 C048806900027
6.000 3.12E+2 8.20E+1 C048806900028
6.500 4.87E+2 1.59E+2 C048806900029
7.000 7.12E+2 2.80E+2 C048806900030
ENDDATA 12 0 C048806900031
ENDSUBENT 30 0 C048806999999
SUBENT C0488070 20160323 C158C048807000001
BIB 5 13 C048807000002
REACTION (46-PD-102(P,G)47-AG-103,,SGV) C048807000003
ANALYSIS Thermonuclear reaction rates are usually calculated C048807000004
directly from measured reaction cross sections and C048807000005
level parameters. The relevant quantity is NA <sigma C048807000006
v>T which is Avogadro's number times the average C048807000007
value of the product of the cross section times the C048807000008
velocity, averaged over the Maxwell-Boltzmann C048807000009
velocity distribution at the temperature T of interest.C048807000010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048807000011
their values were added quadratically. C048807000012
STATUS (TABLE) Table III, page 191. C048807000013
(DEP,C0488005) C048807000014
HISTORY (20160323C) BP C048807000015
ENDBIB 13 0 C048807000016
NOCOMMON 0 0 C048807000017
DATA 3 11 C048807000018
KT DATA DATA-ERR C048807000019
K9 CM3/S/MOL CM3/S/MOL C048807000020
3.000 7.87E+1 3.84E+1 C048807000021
3.500 3.19E+2 8.93E+1 C048807000022
4.000 1.00E+3 1.67E+2 C048807000023
4.500 2.62E+3 3.93E+2 C048807000024
5.000 5.98E+3 8.97E+2 C048807000025
5.500 1.22E+4 1.83E+3 C048807000026
6.000 2.28E+4 3.42E+3 C048807000027
6.500 3.94E+4 5.91E+3 C048807000028
7.000 6.36E+4 9.54E+3 C048807000029
7.500 9.73E+4 1.76E+4 C048807000030
8.000 1.42E+5 3.12E+4 C048807000031
ENDDATA 13 0 C048807000032
ENDSUBENT 31 0 C048807099999
SUBENT C0488071 20160323 C158C048807100001
BIB 5 13 C048807100002
REACTION (48-CD-106(P,G)49-IN-107,,SGV) C048807100003
ANALYSIS Thermonuclear reaction rates are usually calculated C048807100004
directly from measured reaction cross sections and C048807100005
level parameters. The relevant quantity is NA <sigma C048807100006
v>T which is Avogadro's number times the average C048807100007
value of the product of the cross section times the C048807100008
velocity, averaged over the Maxwell-Boltzmann C048807100009
velocity distribution at the temperature T of interest.C048807100010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048807100011
their values were added quadratically. C048807100012
STATUS (TABLE) Table III, page 191. C048807100013
(DEP,C0488006) C048807100014
HISTORY (20160323C) BP C048807100015
ENDBIB 13 0 C048807100016
NOCOMMON 0 0 C048807100017
DATA 3 7 C048807100018
KT DATA DATA-ERR C048807100019
K9 CM3/S/MOL CM3/S/MOL C048807100020
4.000 4.12E+2 1.67E+2 C048807100021
4.500 1.06E+3 3.31E+2 C048807100022
5.000 2.31E+3 6.65E+2 C048807100023
5.500 4.43E+3 1.38E+3 C048807100024
6.000 7.70E+3 2.82E+3 C048807100025
6.500 1.23E+4 5.31E+3 C048807100026
7.000 1.85E+4 9.38E+3 C048807100027
ENDDATA 9 0 C048807100028
ENDSUBENT 27 0 C048807199999
SUBENT C0488072 20160323 C158C048807200001
BIB 5 13 C048807200002
REACTION (48-CD-108(P,G)49-IN-109,,SGV) C048807200003
ANALYSIS Thermonuclear reaction rates are usually calculated C048807200004
directly from measured reaction cross sections and C048807200005
level parameters. The relevant quantity is NA <sigma C048807200006
v>T which is Avogadro's number times the average C048807200007
value of the product of the cross section times the C048807200008
velocity, averaged over the Maxwell-Boltzmann C048807200009
velocity distribution at the temperature T of interest.C048807200010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048807200011
their values were added quadratically. C048807200012
STATUS (TABLE) Table III, page 191. C048807200013
(DEP,C0488007) C048807200014
HISTORY (20160323C) BP C048807200015
ENDBIB 13 0 C048807200016
NOCOMMON 0 0 C048807200017
DATA 3 6 C048807200018
KT DATA DATA-ERR C048807200019
K9 CM3/S/MOL CM3/S/MOL C048807200020
4.000 8.01E+2 3.72E+2 C048807200021
4.500 2.05E+3 7.32E+2 C048807200022
5.000 4.47E+3 1.48E+3 C048807200023
5.500 8.62E+3 3.09E+3 C048807200024
6.000 1.50E+4 6.29E+3 C048807200025
6.500 2.42E+4 1.20E+4 C048807200026
ENDDATA 8 0 C048807200027
ENDSUBENT 26 0 C048807299999
SUBENT C0488073 20160323 C158C048807300001
BIB 5 13 C048807300002
REACTION (48-CD-114(P,G)49-IN-115-M,,SGV) C048807300003
ANALYSIS Thermonuclear reaction rates are usually calculated C048807300004
directly from measured reaction cross sections and C048807300005
level parameters. The relevant quantity is NA <sigma C048807300006
v>T which is Avogadro's number times the average C048807300007
value of the product of the cross section times the C048807300008
velocity, averaged over the Maxwell-Boltzmann C048807300009
velocity distribution at the temperature T of interest.C048807300010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048807300011
their values were added quadratically. C048807300012
STATUS (TABLE) Table III, page 191. C048807300013
(DEP,C0488008) C048807300014
HISTORY (20160323C) BP C048807300015
ENDBIB 13 0 C048807300016
NOCOMMON 0 0 C048807300017
DATA 3 5 C048807300018
KT DATA DATA-ERR C048807300019
K9 CM3/S/MOL CM3/S/MOL C048807300020
6.000 1.23E+3 6.06E+2 C048807300021
6.500 1.78E+3 7.99E+2 C048807300022
7.000 2.45E+3 1.06E+3 C048807300023
7.500 3.23E+3 1.40E+3 C048807300024
8.000 4.12E+3 1.87E+3 C048807300025
ENDDATA 7 0 C048807300026
ENDSUBENT 25 0 C048807399999
SUBENT C0488074 20160323 C158C048807400001
BIB 5 13 C048807400002
REACTION (48-CD-116(P,G)49-IN-117-M,,SGV) C048807400003
ANALYSIS Thermonuclear reaction rates are usually calculated C048807400004
directly from measured reaction cross sections and C048807400005
level parameters. The relevant quantity is NA <sigma C048807400006
v>T which is Avogadro's number times the average C048807400007
value of the product of the cross section times the C048807400008
velocity, averaged over the Maxwell-Boltzmann C048807400009
velocity distribution at the temperature T of interest.C048807400010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048807400011
their values were added quadratically. C048807400012
STATUS (TABLE) Table III, page 191. C048807400013
(DEP,C0488009) C048807400014
HISTORY (20160323C) BP C048807400015
ENDBIB 13 0 C048807400016
NOCOMMON 0 0 C048807400017
DATA 3 6 C048807400018
KT DATA DATA-ERR C048807400019
K9 CM3/S/MOL CM3/S/MOL C048807400020
3.500 2.38E+0 1.02E+0 C048807400021
4.000 7.94E+0 2.46E+0 C048807400022
4.500 2.11E+1 5.90E+0 C048807400023
5.000 4.76E+1 1.50E+1 C048807400024
5.500 9.40E+1 3.66E+1 C048807400025
6.000 1.67E+2 8.02E+1 C048807400026
ENDDATA 8 0 C048807400027
ENDSUBENT 26 0 C048807499999
SUBENT C0488075 20160324 C158C048807500001
BIB 5 13 C048807500002
REACTION (50-SN-112(P,G)51-SB-113,,SGV) C048807500003
ANALYSIS Thermonuclear reaction rates are usually calculated C048807500004
directly from measured reaction cross sections and C048807500005
level parameters. The relevant quantity is NA <sigma C048807500006
v>T which is Avogadro's number times the average C048807500007
value of the product of the cross section times the C048807500008
velocity, averaged over the Maxwell-Boltzmann C048807500009
velocity distribution at the temperature T of interest.C048807500010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048807500011
their values were added quadratically. C048807500012
STATUS (TABLE) Table III, page 192. C048807500013
(DEP,C0488010) C048807500014
HISTORY (20160324C) BP C048807500015
ENDBIB 13 0 C048807500016
NOCOMMON 0 0 C048807500017
DATA 3 5 C048807500018
KT DATA DATA-ERR C048807500019
K9 CM3/S/MOL CM3/S/MOL C048807500020
3.500 2.29E+2 1.15E+2 C048807500021
4.000 6.90E+2 3.21E+2 C048807500022
4.500 1.62E+3 7.94E+2 C048807500023
5.000 3.20E+3 1.76E+3 C048807500024
5.500 5.54E+3 3.50E+3 C048807500025
ENDDATA 7 0 C048807500026
ENDSUBENT 25 0 C048807599999
SUBENT C0488076 20160324 C158C048807600001
BIB 5 13 C048807600002
REACTION (62-SM-144(P,G)63-EU-145,,SGV) C048807600003
ANALYSIS Thermonuclear reaction rates are usually calculated C048807600004
directly from measured reaction cross sections and C048807600005
level parameters. The relevant quantity is NA <sigma C048807600006
v>T which is Avogadro's number times the average C048807600007
value of the product of the cross section times the C048807600008
velocity, averaged over the Maxwell-Boltzmann C048807600009
velocity distribution at the temperature T of interest.C048807600010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048807600011
their values were added quadratically. C048807600012
STATUS (TABLE) Table III, page 192. C048807600013
(DEP,C0488011) C048807600014
HISTORY (20160324C) BP C048807600015
ENDBIB 13 0 C048807600016
NOCOMMON 0 0 C048807600017
DATA 3 10 C048807600018
KT DATA DATA-ERR C048807600019
K9 CM3/S/MOL CM3/S/MOL C048807600020
3.500 2.70E+1 1.34E+1 C048807600021
4.000 9.06E+1 3.35E+1 C048807600022
4.500 2.41E+2 6.92E+1 C048807600023
5.000 5.50E+2 1.10E+2 C048807600024
5.500 1.13E+3 1.85E+2 C048807600025
6.000 2.14E+3 3.45E+2 C048807600026
6.500 3.79E+3 7.19E+2 C048807600027
7.000 6.31E+3 1.49E+3 C048807600028
7.500 9.96E+3 2.93E+3 C048807600029
8.000 1.50E+4 5.34E+3 C048807600030
ENDDATA 12 0 C048807600031
ENDSUBENT 30 0 C048807699999
SUBENT C0488077 20160324 C158C048807700001
BIB 5 13 C048807700002
REACTION (30-ZN-68(P,N)31-GA-68,,SGV) C048807700003
ANALYSIS Thermonuclear reaction rates are usually calculated C048807700004
directly from measured reaction cross sections and C048807700005
level parameters. The relevant quantity is NA <sigma C048807700006
v>T which is Avogadro's number times the average C048807700007
value of the product of the cross section times the C048807700008
velocity, averaged over the Maxwell-Boltzmann C048807700009
velocity distribution at the temperature T of interest.C048807700010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048807700011
their values were added quadratically. C048807700012
STATUS (TABLE) Table III, page 192. C048807700013
(DEP,C0487025) C048807700014
HISTORY (20160324C) BP C048807700015
ENDBIB 13 0 C048807700016
NOCOMMON 0 0 C048807700017
DATA 3 5 C048807700018
KT DATA DATA-ERR C048807700019
K9 CM3/S/MOL CM3/S/MOL C048807700020
3.000 1.63E+2 2.55E+1 C048807700021
3.500 1.34E+3 2.71E+2 C048807700022
4.000 6.47E+3 1.74E+3 C048807700023
4.500 2.18E+4 7.55E+3 C048807700024
5.000 5.65E+4 2.45E+4 C048807700025
ENDDATA 7 0 C048807700026
ENDSUBENT 25 0 C048807799999
SUBENT C0488078 20160324 C158C048807800001
BIB 5 13 C048807800002
REACTION (32-GE-74(P,N)33-AS-74,,SGV) C048807800003
ANALYSIS Thermonuclear reaction rates are usually calculated C048807800004
directly from measured reaction cross sections and C048807800005
level parameters. The relevant quantity is NA <sigma C048807800006
v>T which is Avogadro's number times the average C048807800007
value of the product of the cross section times the C048807800008
velocity, averaged over the Maxwell-Boltzmann C048807800009
velocity distribution at the temperature T of interest.C048807800010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048807800011
their values were added quadratically. C048807800012
STATUS (TABLE) Table III, page 192. C048807800013
(DEP,C0487026) C048807800014
HISTORY (20160324C) BP C048807800015
ENDBIB 13 0 C048807800016
NOCOMMON 0 0 C048807800017
DATA 3 10 C048807800018
KT DATA DATA-ERR C048807800019
K9 CM3/S/MOL CM3/S/MOL C048807800020
2.500 3.61E+1 5.41E+0 C048807800021
3.000 5.28E+2 7.92E+1 C048807800022
3.500 3.61E+3 5.42E+2 C048807800023
4.000 1.53E+4 2.30E+3 C048807800024
4.500 4.67E+4 7.75E+3 C048807800025
5.000 1.13E+5 2.50E+4 C048807800026
5.500 2.33E+5 6.52E+4 C048807800027
6.000 4.22E+5 1.44E+5 C048807800028
6.500 6.92E+5 2.82E+5 C048807800029
7.000 1.05E+6 4.96E+6 C048807800030
ENDDATA 12 0 C048807800031
ENDSUBENT 30 0 C048807899999
SUBENT C0488079 20160324 C158C048807900001
BIB 5 13 C048807900002
REACTION (32-GE-76(P,N)33-AS-76,,SGV) C048807900003
ANALYSIS Thermonuclear reaction rates are usually calculated C048807900004
directly from measured reaction cross sections and C048807900005
level parameters. The relevant quantity is NA <sigma C048807900006
v>T which is Avogadro's number times the average C048807900007
value of the product of the cross section times the C048807900008
velocity, averaged over the Maxwell-Boltzmann C048807900009
velocity distribution at the temperature T of interest.C048807900010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048807900011
their values were added quadratically. C048807900012
STATUS (TABLE) Table III, page 192. C048807900013
(DEP,C0487027) C048807900014
HISTORY (20160324C) BP C048807900015
ENDBIB 13 0 C048807900016
NOCOMMON 0 0 C048807900017
DATA 3 11 C048807900018
KT DATA DATA-ERR C048807900019
K9 CM3/S/MOL CM3/S/MOL C048807900020
2.000 9.04E+1 2.29E+1 C048807900021
2.500 1.10E+3 1.65E+2 C048807900022
3.000 6.35E+3 9.53E+2 C048807900023
3.500 2.40E+4 3.60E+3 C048807900024
4.000 6.86E+4 1.03E+4 C048807900025
4.500 1.61E+5 2.42E+4 C048807900026
5.000 3.26E+5 4.89E+4 C048807900027
5.500 5.87E+5 9.59E+4 C048807900028
6.000 9.66E+5 2.05E+5 C048807900029
6.500 1.45E+6 3.94E+5 C048807900030
7.000 2.13E+6 6.91E+5 C048807900031
ENDDATA 13 0 C048807900032
ENDSUBENT 31 0 C048807999999
SUBENT C0488080 20160324 C158C048808000001
BIB 5 13 C048808000002
REACTION (38-SR-87(P,N)39-Y-87,,SGV) C048808000003
ANALYSIS Thermonuclear reaction rates are usually calculated C048808000004
directly from measured reaction cross sections and C048808000005
level parameters. The relevant quantity is NA <sigma C048808000006
v>T which is Avogadro's number times the average C048808000007
value of the product of the cross section times the C048808000008
velocity, averaged over the Maxwell-Boltzmann C048808000009
velocity distribution at the temperature T of interest.C048808000010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048808000011
their values were added quadratically. C048808000012
STATUS (TABLE) Table III, page 192. C048808000013
(DEP,C0488012) C048808000014
HISTORY (20160324C) BP C048808000015
ENDBIB 13 0 C048808000016
NOCOMMON 0 0 C048808000017
DATA 3 11 C048808000018
KT DATA DATA-ERR C048808000019
K9 CM3/S/MOL CM3/S/MOL C048808000020
3.000 3.84E+2 5.76E+1 C048808000021
3.500 1.75E+3 2.63E+2 C048808000022
4.000 5.81E+3 8.72E+2 C048808000023
4.500 1.55E+4 2.33E+3 C048808000024
5.000 3.50E+4 5.25E+3 C048808000025
5.500 6.93E+4 1.04E+4 C048808000026
6.000 1.24E+5 1.86E+4 C048808000027
6.500 2.03E+5 3.82E+4 C048808000028
7.000 3.12E+5 7.33E+4 C048808000029
7.500 4.53E+5 1.29E+5 C048808000030
8.000 6.27E+5 2.11E+5 C048808000031
ENDDATA 13 0 C048808000032
ENDSUBENT 31 0 C048808099999
SUBENT C0488081 20160324 C158C048808100001
BIB 5 13 C048808100002
REACTION (38-SR-88(P,N)39-Y-88,,SGV) C048808100003
ANALYSIS Thermonuclear reaction rates are usually calculated C048808100004
directly from measured reaction cross sections and C048808100005
level parameters. The relevant quantity is NA <sigma C048808100006
v>T which is Avogadro's number times the average C048808100007
value of the product of the cross section times the C048808100008
velocity, averaged over the Maxwell-Boltzmann C048808100009
velocity distribution at the temperature T of interest.C048808100010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048808100011
their values were added quadratically. C048808100012
STATUS (TABLE) Table III, page 192. C048808100013
(DEP,C0488013) C048808100014
HISTORY (20160324C) BP C048808100015
ENDBIB 13 0 C048808100016
NOCOMMON 0 0 C048808100017
DATA 3 5 C048808100018
KT DATA DATA-ERR C048808100019
K9 CM3/S/MOL CM3/S/MOL C048808100020
2.000 1.86E-3 2.79E-4 C048808100021
2.500 4.25E-1 6.76E-2 C048808100022
3.000 1.61E+1 4.67E+0 C048808100023
3.500 2.18E+2 9.68E+1 C048808100024
4.000 1.53E+3 9.38E+2 C048808100025
ENDDATA 7 0 C048808100026
ENDSUBENT 25 0 C048808199999
SUBENT C0488082 20160324 C158C048808200001
BIB 5 13 C048808200002
REACTION (40-ZR-94(P,N)41-NB-94-M,,SGV) C048808200003
ANALYSIS Thermonuclear reaction rates are usually calculated C048808200004
directly from measured reaction cross sections and C048808200005
level parameters. The relevant quantity is NA <sigma C048808200006
v>T which is Avogadro's number times the average C048808200007
value of the product of the cross section times the C048808200008
velocity, averaged over the Maxwell-Boltzmann C048808200009
velocity distribution at the temperature T of interest.C048808200010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048808200011
their values were added quadratically. C048808200012
STATUS (TABLE) Table III, page 192. C048808200013
(DEP,C0488014) C048808200014
HISTORY (20160324C) BP C048808200015
ENDBIB 13 0 C048808200016
NOCOMMON 0 0 C048808200017
DATA 3 10 C048808200018
KT DATA DATA-ERR C048808200019
K9 CM3/S/MOL CM3/S/MOL C048808200020
3.500 6.37E+3 2.01E+3 C048808200021
4.000 2.21E+4 4.94E+3 C048808200022
4.500 6.06E+4 9.09E+3 C048808200023
5.000 1.40E+5 2.10E+4 C048808200024
5.500 2.85E+5 4.28E+4 C048808200025
6.000 5.21E+5 7.82E+4 C048808200026
6.500 8.77E+5 1.66E+5 C048808200027
7.000 1.30E+6 3.24E+5 C048808200028
7.500 2.04E+6 6.34E+5 C048808200029
8.000 2.88E+6 1.03E+6 C048808200030
ENDDATA 12 0 C048808200031
ENDSUBENT 30 0 C048808299999
SUBENT C0488083 20160324 C158C048808300001
BIB 5 13 C048808300002
REACTION (40-ZR-96(P,N)41-NB-96,,SGV) C048808300003
ANALYSIS Thermonuclear reaction rates are usually calculated C048808300004
directly from measured reaction cross sections and C048808300005
level parameters. The relevant quantity is NA <sigma C048808300006
v>T which is Avogadro's number times the average C048808300007
value of the product of the cross section times the C048808300008
velocity, averaged over the Maxwell-Boltzmann C048808300009
velocity distribution at the temperature T of interest.C048808300010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048808300011
their values were added quadratically. C048808300012
STATUS (TABLE) Table III, page 192. C048808300013
(DEP,C0488015) C048808300014
HISTORY (20160324C) BP C048808300015
ENDBIB 13 0 C048808300016
NOCOMMON 0 0 C048808300017
DATA 3 10 C048808300018
KT DATA DATA-ERR C048808300019
K9 CM3/S/MOL CM3/S/MOL C048808300020
3.500 2.36E+3 9.92E+2 C048808300021
4.000 8.21E+3 2.39E+3 C048808300022
4.500 2.28E+4 4.21E+3 C048808300023
5.000 5.37E+4 1.14E+4 C048808300024
5.500 1.11E+5 1.76E+4 C048808300025
6.000 2.07E+5 4.01E+4 C048808300026
6.500 3.55E+5 8.64E+4 C048808300027
7.000 5.66E+5 1.70E+5 C048808300028
7.500 8.50E+5 3.34E+5 C048808300029
8.000 1.22E+6 5.50E+5 C048808300030
ENDDATA 12 0 C048808300031
ENDSUBENT 30 0 C048808399999
SUBENT C0488084 20160324 C158C048808400001
BIB 5 13 C048808400002
REACTION (42-MO-95(P,N)43-TC-95,,SGV) C048808400003
ANALYSIS Thermonuclear reaction rates are usually calculated C048808400004
directly from measured reaction cross sections and C048808400005
level parameters. The relevant quantity is NA <sigma C048808400006
v>T which is Avogadro's number times the average C048808400007
value of the product of the cross section times the C048808400008
velocity, averaged over the Maxwell-Boltzmann C048808400009
velocity distribution at the temperature T of interest.C048808400010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048808400011
their values were added quadratically. C048808400012
STATUS (TABLE) Table III, page 192. C048808400013
(DEP,C0487028) C048808400014
HISTORY (20160324C) BP C048808400015
ENDBIB 13 0 C048808400016
NOCOMMON 0 0 C048808400017
DATA 3 7 C048808400018
KT DATA DATA-ERR C048808400019
K9 CM3/S/MOL CM3/S/MOL C048808400020
2.500 1.04E+1 4.50E+0 C048808400021
3.000 1.03E+2 2.77E+1 C048808400022
3.500 5.49E+2 1.20E+2 C048808400023
4.000 1.98E+3 4.60E+2 C048808400024
4.500 5.45E+3 1.59E+3 C048808400025
5.000 1.23E+4 4.57E+3 C048808400026
5.500 2.40E+4 1.11E+4 C048808400027
ENDDATA 9 0 C048808400028
ENDSUBENT 27 0 C048808499999
SUBENT C0488085 20160324 C158C048808500001
BIB 5 13 C048808500002
REACTION (42-MO-95(P,N)43-TC-95-M,,SGV) C048808500003
ANALYSIS Thermonuclear reaction rates are usually calculated C048808500004
directly from measured reaction cross sections and C048808500005
level parameters. The relevant quantity is NA <sigma C048808500006
v>T which is Avogadro's number times the average C048808500007
value of the product of the cross section times the C048808500008
velocity, averaged over the Maxwell-Boltzmann C048808500009
velocity distribution at the temperature T of interest.C048808500010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048808500011
their values were added quadratically. C048808500012
STATUS (TABLE) Table III, page 192. C048808500013
(DEP,C0487029) C048808500014
HISTORY (20160324C) BP C048808500015
ENDBIB 13 0 C048808500016
NOCOMMON 0 0 C048808500017
DATA 3 6 C048808500018
KT DATA DATA-ERR C048808500019
K9 CM3/S/MOL CM3/S/MOL C048808500020
2.500 2.12E+1 8.55E+0 C048808500021
3.000 2.20E+2 6.50E+1 C048808500022
3.500 1.19E+3 3.20E+2 C048808500023
4.000 4.27E+3 1.32E+3 C048808500024
4.500 1.16E+4 4.48E+3 C048808500025
5.000 2.57E+4 1.25E+4 C048808500026
ENDDATA 8 0 C048808500027
ENDSUBENT 26 0 C048808599999
SUBENT C0488086 20160324 C158C048808600001
BIB 5 13 C048808600002
REACTION (42-MO-96(P,N)43-TC-96,,SGV) C048808600003
ANALYSIS Thermonuclear reaction rates are usually calculated C048808600004
directly from measured reaction cross sections and C048808600005
level parameters. The relevant quantity is NA <sigma C048808600006
v>T which is Avogadro's number times the average C048808600007
value of the product of the cross section times the C048808600008
velocity, averaged over the Maxwell-Boltzmann C048808600009
velocity distribution at the temperature T of interest.C048808600010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048808600011
their values were added quadratically. C048808600012
STATUS (TABLE) Table III, page 192. C048808600013
(DEP,C0487030) C048808600014
HISTORY (20160324C) BP C048808600015
ENDBIB 13 0 C048808600016
NOCOMMON 0 0 C048808600017
DATA 3 10 C048808600018
KT DATA DATA-ERR C048808600019
K9 CM3/S/MOL CM3/S/MOL C048808600020
2.000 1.83E-2 2.74E-3 C048808600021
2.500 1.58E+0 2.37E-1 C048808600022
3.000 3.14E+1 4.71E+0 C048808600023
3.500 2.65E+2 5.67E+1 C048808600024
4.000 1.30E+3 3.90E+2 C048808600025
4.500 4.46E+3 1.75E+3 C048808600026
5.000 1.18E+4 5.77E+3 C048808600027
5.500 2.59E+4 1.53E+4 C048808600028
6.000 4.96E+4 3.43E+4 C048808600029
6.500 8.52E+4 6.78E+4 C048808600030
ENDDATA 12 0 C048808600031
ENDSUBENT 30 0 C048808699999
SUBENT C0488087 20160324 C158C048808700001
BIB 5 13 C048808700002
REACTION (42-MO-96(P,N)43-TC-96-M,,SGV) C048808700003
ANALYSIS Thermonuclear reaction rates are usually calculated C048808700004
directly from measured reaction cross sections and C048808700005
level parameters. The relevant quantity is NA <sigma C048808700006
v>T which is Avogadro's number times the average C048808700007
value of the product of the cross section times the C048808700008
velocity, averaged over the Maxwell-Boltzmann C048808700009
velocity distribution at the temperature T of interest.C048808700010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048808700011
their values were added quadratically. C048808700012
STATUS (TABLE) Table III, page 192. C048808700013
(DEP,C0487031) C048808700014
HISTORY (20160324C) BP C048808700015
ENDBIB 13 0 C048808700016
NOCOMMON 0 0 C048808700017
DATA 3 7 C048808700018
KT DATA DATA-ERR C048808700019
K9 CM3/S/MOL CM3/S/MOL C048808700020
2.000 8.46E-3 1.27E-3 C048808700021
2.500 7.51E-1 1.13E-1 C048808700022
3.000 1.51E-1 2.27E+0 C048808700023
3.500 1.28E+2 2.66E+1 C048808700024
4.000 6.34E+2 1.85E+2 C048808700025
4.500 2.17E+3 8.27E+2 C048808700026
5.000 5.75E+3 2.72E+3 C048808700027
ENDDATA 9 0 C048808700028
ENDSUBENT 27 0 C048808799999
SUBENT C0488088 20160324 C158C048808800001
BIB 5 13 C048808800002
REACTION (46-PD-104(P,N)47-AG-104,,SGV) C048808800003
ANALYSIS Thermonuclear reaction rates are usually calculated C048808800004
directly from measured reaction cross sections and C048808800005
level parameters. The relevant quantity is NA <sigma C048808800006
v>T which is Avogadro's number times the average C048808800007
value of the product of the cross section times the C048808800008
velocity, averaged over the Maxwell-Boltzmann C048808800009
velocity distribution at the temperature T of interest.C048808800010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048808800011
their values were added quadratically. C048808800012
STATUS (TABLE) Table III, page 192. C048808800013
(DEP,C0488016) C048808800014
HISTORY (20160324C) BP C048808800015
ENDBIB 13 0 C048808800016
NOCOMMON 0 0 C048808800017
DATA 3 5 C048808800018
KT DATA DATA-ERR C048808800019
K9 CM3/S/MOL CM3/S/MOL C048808800020
2.000 1.48E-5 2.22E-6 C048808800021
2.500 6.01E-3 1.11E-3 C048808800022
3.000 3.24E-1 9.56E-2 C048808800023
3.500 5.50E+0 2.28E+0 C048808800024
4.000 4.51E+1 2.44E+1 C048808800025
ENDDATA 7 0 C048808800026
ENDSUBENT 25 0 C048808899999
SUBENT C0488089 20160324 C158C048808900001
BIB 5 13 C048808900002
REACTION (46-PD-105(P,N)47-AG-105,,SGV) C048808900003
ANALYSIS Thermonuclear reaction rates are usually calculated C048808900004
directly from measured reaction cross sections and C048808900005
level parameters. The relevant quantity is NA <sigma C048808900006
v>T which is Avogadro's number times the average C048808900007
value of the product of the cross section times the C048808900008
velocity, averaged over the Maxwell-Boltzmann C048808900009
velocity distribution at the temperature T of interest.C048808900010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048808900011
their values were added quadratically. C048808900012
STATUS (TABLE) Table III, page 192. C048808900013
(DEP,C0488017) C048808900014
HISTORY (20160324C) BP C048808900015
ENDBIB 13 0 C048808900016
NOCOMMON 0 0 C048808900017
DATA 3 11 C048808900018
KT DATA DATA-ERR C048808900019
K9 CM3/S/MOL CM3/S/MOL C048808900020
3.000 6.59E+1 2.60E+1 C048808900021
3.500 4.37E+2 1.18E+2 C048808900022
4.000 1.89E+3 3.27E+2 C048808900023
4.500 6.09E+3 9.14E+2 C048808900024
5.000 1.59E+4 2.39E+3 C048808900025
5.500 3.53E+4 6.06E+3 C048808900026
6.000 6.90E+4 1.50E+4 C048808900027
6.500 1.22E+5 3.29E+4 C048808900028
7.000 2.00E+5 7.17E+4 C048808900029
7.500 3.06E+5 1.27E+5 C048808900030
8.000 4.44E+5 2.10E+5 C048808900031
ENDDATA 13 0 C048808900032
ENDSUBENT 31 0 C048808999999
SUBENT C0488090 20160324 C158C048809000001
BIB 5 13 C048809000002
REACTION (46-PD-106(P,N)47-AG-106,,SGV) C048809000003
ANALYSIS Thermonuclear reaction rates are usually calculated C048809000004
directly from measured reaction cross sections and C048809000005
level parameters. The relevant quantity is NA <sigma C048809000006
v>T which is Avogadro's number times the average C048809000007
value of the product of the cross section times the C048809000008
velocity, averaged over the Maxwell-Boltzmann C048809000009
velocity distribution at the temperature T of interest.C048809000010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048809000011
their values were added quadratically. C048809000012
STATUS (TABLE) Table III, page 192. C048809000013
(DEP,C0488018) C048809000014
HISTORY (20160324C) BP C048809000015
ENDBIB 13 0 C048809000016
NOCOMMON 0 0 C048809000017
DATA 3 11 C048809000018
KT DATA DATA-ERR C048809000019
K9 CM3/S/MOL CM3/S/MOL C048809000020
2.500 2.87E+0 4.31E-1 C048809000021
3.000 5.99E+1 8.99E+0 C048809000022
3.500 5.56E+2 8.34E+1 C048809000023
4.000 3.05E+3 4.58E+2 C048809000024
4.500 1.17E+4 1.76E+3 C048809000025
5.000 3.43E+4 6.04E+3 C048809000026
5.500 8.32E+4 1.95E+4 C048809000027
6.000 1.74E+5 5.13E+4 C048809000028
6.500 3.23E+5 1.16E+5 C048809000029
7.000 5.49E+5 2.35E+5 C048809000030
7.500 8.66E+5 4.30E+5 C048809000031
ENDDATA 13 0 C048809000032
ENDSUBENT 31 0 C048809099999
SUBENT C0488091 20160324 C158C048809100001
BIB 5 13 C048809100002
REACTION (46-PD-106(P,N)47-AG-106-M,,SGV) C048809100003
ANALYSIS Thermonuclear reaction rates are usually calculated C048809100004
directly from measured reaction cross sections and C048809100005
level parameters. The relevant quantity is NA <sigma C048809100006
v>T which is Avogadro's number times the average C048809100007
value of the product of the cross section times the C048809100008
velocity, averaged over the Maxwell-Boltzmann C048809100009
velocity distribution at the temperature T of interest.C048809100010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048809100011
their values were added quadratically. C048809100012
STATUS (TABLE) Table III, page 192. C048809100013
(DEP,C0488019) C048809100014
HISTORY (20160324C) BP C048809100015
ENDBIB 13 0 C048809100016
NOCOMMON 0 0 C048809100017
DATA 3 12 C048809100018
KT DATA DATA-ERR C048809100019
K9 CM3/S/MOL CM3/S/MOL C048809100020
2.500 4.84E-2 7.26E-3 C048809100021
3.000 8.80E-1 1.32E-1 C048809100022
3.500 7.09E+0 1.06E+0 C048809100023
4.000 3.44E+1 5.16E+0 C048809100024
4.500 1.19E+2 1.79E+1 C048809100025
5.000 3.23E+2 4.85E+1 C048809100026
5.500 7.34E+2 1.17E+2 C048809100027
6.000 1.46E+3 3.05E+2 C048809100028
6.500 2.60E+3 6.82E+2 C048809100029
7.000 4.28E+3 1.36E+3 C048809100030
7.500 6.57E+3 2.49E+3 C048809100031
8.000 9.54E+3 4.21E+3 C048809100032
ENDDATA 14 0 C048809100033
ENDSUBENT 32 0 C048809199999
SUBENT C0488092 20160324 C158C048809200001
BIB 5 13 C048809200002
REACTION (48-CD-116(P,N)49-IN-116-M,,SGV) C048809200003
ANALYSIS Thermonuclear reaction rates are usually calculated C048809200004
directly from measured reaction cross sections and C048809200005
level parameters. The relevant quantity is NA <sigma C048809200006
v>T which is Avogadro's number times the average C048809200007
value of the product of the cross section times the C048809200008
velocity, averaged over the Maxwell-Boltzmann C048809200009
velocity distribution at the temperature T of interest.C048809200010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048809200011
their values were added quadratically. C048809200012
STATUS (TABLE) Table III, page 193. C048809200013
(DEP,C0488020) C048809200014
HISTORY (20160324C) BP C048809200015
ENDBIB 13 0 C048809200016
NOCOMMON 0 0 C048809200017
DATA 3 7 C048809200018
KT DATA DATA-ERR C048809200019
KEV CM3/S/MOL CM3/S/MOL C048809200020
2.500 1.54E+0 6.77E-1 C048809200021
3.000 1.51E+1 3.54E+0 C048809200022
3.500 8.62E+1 1.43E+1 C048809200023
4.000 3.40E+2 6.61E+1 C048809200024
4.500 1.03E+3 2.79E+2 C048809200025
5.000 2.53E+3 1.02E+3 C048809200026
5.500 5.33E+3 2.64E+3 C048809200027
ENDDATA 9 0 C048809200028
ENDSUBENT 27 0 C048809299999
SUBENT C0488093 20160324 C158C048809300001
BIB 5 13 C048809300002
REACTION (50-SN-115(P,N)51-SB-115,,SGV) C048809300003
ANALYSIS Thermonuclear reaction rates are usually calculated C048809300004
directly from measured reaction cross sections and C048809300005
level parameters. The relevant quantity is NA <sigma C048809300006
v>T which is Avogadro's number times the average C048809300007
value of the product of the cross section times the C048809300008
velocity, averaged over the Maxwell-Boltzmann C048809300009
velocity distribution at the temperature T of interest.C048809300010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048809300011
their values were added quadratically. C048809300012
STATUS (TABLE) Table III, page 193. C048809300013
(DEP,C0488021) C048809300014
HISTORY (20160324C) BP C048809300015
ENDBIB 13 0 C048809300016
NOCOMMON 0 0 C048809300017
DATA 3 7 C048809300018
KT DATA DATA-ERR C048809300019
KEV CM3/S/MOL CM3/S/MOL C048809300020
2.500 1.22E-1 6.14E-2 C048809300021
3.000 3.70E+0 1.23E+0 C048809300022
3.500 4.34E+1 1.24E+1 C048809300023
4.000 2.76E+2 8.60E+1 C048809300024
4.500 1.17E+3 4.44E+2 C048809300025
5.000 3.73E+3 1.75E+3 C048809300026
5.500 9.59E+3 5.45E+3 C048809300027
ENDDATA 9 0 C048809300028
ENDSUBENT 27 0 C048809399999
SUBENT C0488094 20160324 C158C048809400001
BIB 5 13 C048809400002
REACTION (50-SN-117(P,N)51-SB-117,,SGV) C048809400003
ANALYSIS Thermonuclear reaction rates are usually calculated C048809400004
directly from measured reaction cross sections and C048809400005
level parameters. The relevant quantity is NA <sigma C048809400006
v>T which is Avogadro's number times the average C048809400007
value of the product of the cross section times the C048809400008
velocity, averaged over the Maxwell-Boltzmann C048809400009
velocity distribution at the temperature T of interest.C048809400010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048809400011
their values were added quadratically. C048809400012
STATUS (TABLE) Table III, page 193. C048809400013
(DEP,C0488022) C048809400014
HISTORY (20160324C) BP C048809400015
ENDBIB 13 0 C048809400016
NOCOMMON 0 0 C048809400017
DATA 3 13 C048809400018
KT DATA DATA-ERR C048809400019
K9 CM3/S/MOL CM3/S/MOL C048809400020
1.500 8.04E-4 3.41E-4 C048809400021
2.000 1.76E-1 3.85E-2 C048809400022
2.500 5.11E+0 7.67E-1 C048809400023
3.000 5.56E+1 8.34E+0 C048809400024
3.500 3.46E+2 5.19E+1 C048809400025
4.000 1.49E+3 2.24E+2 C048809400026
4.500 4.91E+3 7.37E+2 C048809400027
5.000 1.34E+4 2.16E+3 C048809400028
5.500 3.03E+4 6.86E+3 C048809400029
6.000 6.11E+4 1.80E+4 C048809400030
6.500 1.11E+5 4.10E+4 C048809400031
7.000 1.88E+5 8.34E+4 C048809400032
7.500 2.90E+5 1.53E+5 C048809400033
ENDDATA 15 0 C048809400034
ENDSUBENT 33 0 C048809499999
SUBENT C0488095 20160324 C158C048809500001
BIB 5 13 C048809500002
REACTION (50-SN-120(P,N)51-SB-120,,SGV) C048809500003
ANALYSIS Thermonuclear reaction rates are usually calculated C048809500004
directly from measured reaction cross sections and C048809500005
level parameters. The relevant quantity is NA <sigma C048809500006
v>T which is Avogadro's number times the average C048809500007
value of the product of the cross section times the C048809500008
velocity, averaged over the Maxwell-Boltzmann C048809500009
velocity distribution at the temperature T of interest.C048809500010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048809500011
their values were added quadratically. C048809500012
STATUS (TABLE) Table III, page 193. C048809500013
(DEP,C0488023) C048809500014
HISTORY (20160324C) BP C048809500015
ENDBIB 13 0 C048809500016
NOCOMMON 0 0 C048809500017
DATA 3 12 C048809500018
KT DATA DATA-ERR C048809500019
K9 CM3/S/MOL CM3/S/MOL C048809500020
2.500 1.14E+0 1.68E-1 C048809500021
3.000 2.03E+1 3.05E+0 C048809500022
3.500 1.70E+2 2.55E+1 C048809500023
4.000 8.67E+2 1.30E+2 C048809500024
4.500 3.13E+3 4.70E+2 C048809500025
5.000 8.80E+3 1.32E+3 C048809500026
5.500 2.06E+4 3.50E+3 C048809500027
6.000 4.17E+4 9.13E+3 C048809500028
6.500 7.59E+4 2.06E+4 C048809500029
7.000 1.26E+5 4.12E+4 C048809500030
7.500 1.90E+5 7.55E+4 C048809500031
8.000 2.87E+5 1.27E+5 C048809500032
ENDDATA 14 0 C048809500033
ENDSUBENT 32 0 C048809599999
SUBENT C0488096 20160324 C158C048809600001
BIB 5 13 C048809600002
REACTION (50-SN-122(P,N)51-SB-122,,SGV) C048809600003
ANALYSIS Thermonuclear reaction rates are usually calculated C048809600004
directly from measured reaction cross sections and C048809600005
level parameters. The relevant quantity is NA <sigma C048809600006
v>T which is Avogadro's number times the average C048809600007
value of the product of the cross section times the C048809600008
velocity, averaged over the Maxwell-Boltzmann C048809600009
velocity distribution at the temperature T of interest.C048809600010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048809600011
their values were added quadratically. C048809600012
STATUS (TABLE) Table III, page 193. C048809600013
(DEP,C0488024) C048809600014
HISTORY (20160324C) BP C048809600015
ENDBIB 13 0 C048809600016
NOCOMMON 0 0 C048809600017
DATA 3 7 C048809600018
KT DATA DATA-ERR C048809600019
K9 CM3/S/MOL CM3/S/MOL C048809600020
4.000 9.90E+2 1.49E+2 C048809600021
4.500 3.35E+3 5.03E+2 C048809600022
5.000 9.07E+3 1.56E+3 C048809600023
5.500 2.00E+4 4.69E+3 C048809600024
6.000 4.19E+4 1.12E+4 C048809600025
6.500 7.62E+4 2.96E+4 C048809600026
7.000 1.27E+4 5.78E+4 C048809600027
ENDDATA 9 0 C048809600028
ENDSUBENT 27 0 C048809699999
SUBENT C0488097 20160324 C158C048809700001
BIB 5 13 C048809700002
REACTION (50-SN-124(P,N)51-SB-124,,SGV) C048809700003
ANALYSIS Thermonuclear reaction rates are usually calculated C048809700004
directly from measured reaction cross sections and C048809700005
level parameters. The relevant quantity is NA <sigma C048809700006
v>T which is Avogadro's number times the average C048809700007
value of the product of the cross section times the C048809700008
velocity, averaged over the Maxwell-Boltzmann C048809700009
velocity distribution at the temperature T of interest.C048809700010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048809700011
their values were added quadratically. C048809700012
STATUS (TABLE) Table III, page 193. C048809700013
(DEP,C0488025) C048809700014
HISTORY (20160324C) BP C048809700015
ENDBIB 13 0 C048809700016
NOCOMMON 0 0 C048809700017
DATA 3 9 C048809700018
KT DATA DATA-ERR C048809700019
K9 CM3/S/MOL CM3/S/MOL C048809700020
4.000 1.64E+3 1.13E+3 C048809700021
4.500 5.21E+3 2.58E+3 C048809700022
5.000 1.35E+4 5.49E+3 C048809700023
5.500 2.97E+4 1.09E+4 C048809700024
6.000 5.77E+4 2.11E+4 C048809700025
6.500 1.02E+5 4.00E+4 C048809700026
7.000 1.66E+5 7.29E+4 C048809700027
7.500 2.53E+5 1.26E+5 C048809700028
8.000 3.66E+5 2.06E+5 C048809700029
ENDDATA 11 0 C048809700030
ENDSUBENT 29 0 C048809799999
SUBENT C0488098 20160324 C158C048809800001
BIB 5 13 C048809800002
REACTION (52-TE-123(P,N)53-I-123,,SGV) C048809800003
ANALYSIS Thermonuclear reaction rates are usually calculated C048809800004
directly from measured reaction cross sections and C048809800005
level parameters. The relevant quantity is NA <sigma C048809800006
v>T which is Avogadro's number times the average C048809800007
value of the product of the cross section times the C048809800008
velocity, averaged over the Maxwell-Boltzmann C048809800009
velocity distribution at the temperature T of interest.C048809800010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048809800011
their values were added quadratically. C048809800012
STATUS (TABLE) Table III, page 193. C048809800013
(DEP,C0488026) C048809800014
HISTORY (20160324C) BP C048809800015
ENDBIB 13 0 C048809800016
NOCOMMON 0 0 C048809800017
DATA 3 12 C048809800018
KT DATA DATA-ERR C048809800019
K9 CM3/S/MOL CM3/S/MOL C048809800020
2.500 4.60E+0 9.61E-1 C048809800021
3.000 5.67E+1 8.50E+0 C048809800022
3.500 3.83E+2 5.75E+1 C048809800023
4.000 1.72E+3 2.58E+2 C048809800024
4.500 5.72E+3 8.58E+2 C048809800025
5.000 1.53E+4 2.30E+3 C048809800026
5.500 3.46E+4 5.19E+3 C048809800027
6.000 6.85E+4 1.03E+4 C048809800028
6.500 1.22E+5 1.83E+4 C048809800029
7.000 2.01E+5 3.02E+4 C048809800030
7.500 3.09E+5 5.50E+4 C048809800031
8.000 4.49E+5 9.46E+4 C048809800032
ENDDATA 14 0 C048809800033
ENDSUBENT 32 0 C048809899999
SUBENT C0488099 20160324 C158C048809900001
BIB 5 13 C048809900002
REACTION (52-TE-126(P,N)53-I-126,,SGV) C048809900003
ANALYSIS Thermonuclear reaction rates are usually calculated C048809900004
directly from measured reaction cross sections and C048809900005
level parameters. The relevant quantity is NA <sigma C048809900006
v>T which is Avogadro's number times the average C048809900007
value of the product of the cross section times the C048809900008
velocity, averaged over the Maxwell-Boltzmann C048809900009
velocity distribution at the temperature T of interest.C048809900010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048809900011
their values were added quadratically. C048809900012
STATUS (TABLE) Table III, page 193. C048809900013
(DEP,C0488027) C048809900014
HISTORY (20160324C) BP C048809900015
ENDBIB 13 0 C048809900016
NOCOMMON 0 0 C048809900017
DATA 3 12 C048809900018
KT DATA DATA-ERR C048809900019
K9 CM3/S/MOL CM3/S/MOL C048809900020
2.500 2.01E+0 3.02E-1 C048809900021
3.000 2.49E+1 3.73E+0 C048809900022
3.500 1.68E+2 2.52E+1 C048809900023
4.000 7.55E+2 1.13E+2 C048809900024
4.500 2.54E+3 3.81E+2 C048809900025
5.000 6.91E+3 1.04E+3 C048809900026
5.500 1.59E+4 2.39E+3 C048809900027
6.000 3.21E+4 4.82E+3 C048809900028
6.500 5.84E+4 9.75E+3 C048809900029
7.000 9.77E+4 2.04E+4 C048809900030
7.500 1.53E+5 3.87E+4 C048809900031
8.000 2.25E+5 6.73E+4 C048809900032
ENDDATA 14 0 C048809900033
ENDSUBENT 32 0 C048809999999
SUBENT C0488100 20160324 C158C048810000001
BIB 5 13 C048810000002
REACTION (52-TE-128(P,N)53-I-128,,SGV) C048810000003
ANALYSIS Thermonuclear reaction rates are usually calculated C048810000004
directly from measured reaction cross sections and C048810000005
level parameters. The relevant quantity is NA <sigma C048810000006
v>T which is Avogadro's number times the average C048810000007
value of the product of the cross section times the C048810000008
velocity, averaged over the Maxwell-Boltzmann C048810000009
velocity distribution at the temperature T of interest.C048810000010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048810000011
their values were added quadratically. C048810000012
STATUS (TABLE) Table III, page 193. C048810000013
(DEP,C0488028) C048810000014
HISTORY (20160324C) BP C048810000015
ENDBIB 13 0 C048810000016
NOCOMMON 0 0 C048810000017
DATA 3 12 C048810000018
KT DATA DATA-ERR C048810000019
K9 CM3/S/MOL CM3/S/MOL C048810000020
2.500 1.73E+0 2.59E-1 C048810000021
3.000 1.85E+1 2.78E+0 C048810000022
3.500 1.14E+2 1.71E+1 C048810000023
4.000 4.85E+2 7.28E+1 C048810000024
4.500 1.59E+3 2.39E+2 C048810000025
5.000 4.28E+3 6.42E+2 C048810000026
5.500 9.83E+3 1.47E+3 C048810000027
6.000 1.99E+4 3.44E+3 C048810000028
6.500 3.66E+4 8.31E+3 C048810000029
7.000 6.18E+4 1.76E+4 C048810000030
7.500 9.75E+4 3.35E+4 C048810000031
8.000 1.45E+5 5.89E+4 C048810000032
ENDDATA 14 0 C048810000033
ENDSUBENT 32 0 C048810099999
SUBENT C0488101 20160324 C158C048810100001
BIB 5 13 C048810100002
REACTION (52-TE-130(P,N)53-I-130,,SGV) C048810100003
ANALYSIS Thermonuclear reaction rates are usually calculated C048810100004
directly from measured reaction cross sections and C048810100005
level parameters. The relevant quantity is NA <sigma C048810100006
v>T which is Avogadro's number times the average C048810100007
value of the product of the cross section times the C048810100008
velocity, averaged over the Maxwell-Boltzmann C048810100009
velocity distribution at the temperature T of interest.C048810100010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048810100011
their values were added quadratically. C048810100012
STATUS (TABLE) Table III, page 193. C048810100013
(DEP,C0488029) C048810100014
HISTORY (20160324C) BP C048810100015
ENDBIB 13 0 C048810100016
NOCOMMON 0 0 C048810100017
DATA 3 12 C048810100018
KT DATA DATA-ERR C048810100019
K9 CM3/S/MOL CM3/S/MOL C048810100020
2.500 2.86E+0 9.67E-1 C048810100021
3.000 2.72E+1 4.27E+0 C048810100022
3.500 1.60E+2 2.40E+1 C048810100023
4.000 6.79E+2 1.02E+2 C048810100024
4.500 2.24E+3 3.36E+2 C048810100025
5.000 6.04E+3 9.06E+2 C048810100026
5.500 1.40E+4 2.10E+3 C048810100027
6.000 2.84E+4 4.69E+3 C048810100028
6.500 5.22E+4 1.12E+4 C048810100029
7.000 8.83E+4 2.36E+4 C048810100030
7.500 1.39E+5 4.49E+4 C048810100031
8.000 2.08E+5 7.90E+4 C048810100032
ENDDATA 14 0 C048810100033
ENDSUBENT 32 0 C048810199999
SUBENT C0488102 20160324 C158C048810200001
BIB 5 13 C048810200002
REACTION (52-TE-130(P,N)53-I-130-M,,SGV) C048810200003
ANALYSIS Thermonuclear reaction rates are usually calculated C048810200004
directly from measured reaction cross sections and C048810200005
level parameters. The relevant quantity is NA <sigma C048810200006
v>T which is Avogadro's number times the average C048810200007
value of the product of the cross section times the C048810200008
velocity, averaged over the Maxwell-Boltzmann C048810200009
velocity distribution at the temperature T of interest.C048810200010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048810200011
their values were added quadratically. C048810200012
STATUS (TABLE) Table III, page 193. C048810200013
(DEP,C0488030) C048810200014
HISTORY (20160324C) BP C048810200015
ENDBIB 13 0 C048810200016
NOCOMMON 0 0 C048810200017
DATA 3 12 C048810200018
KT DATA DATA-ERR C048810200019
K9 CM3/S/MOL CM3/S/MOL C048810200020
2.500 6.81E+0 3.34E+0 C048810200021
3.000 5.09E+1 1.48E+1 C048810200022
3.500 2.31E+2 4.07E+1 C048810200023
4.000 7.69E+2 1.15E+2 C048810200024
4.500 2.08E+3 3.12E+2 C048810200025
5.000 4.83E+3 7.25E+2 C048810200026
5.500 9.97E+3 1.50E+3 C048810200027
6.000 1.87E+4 2.81E+3 C048810200028
6.500 3.23E+4 5.72E+3 C048810200029
7.000 5.21E+4 1.20E+4 C048810200030
7.500 7.95E+4 2.30E+4 C048810200031
8.000 1.16E+5 4.05E+4 C048810200032
ENDDATA 14 0 C048810200033
ENDSUBENT 32 0 C048810299999
SUBENT C0488103 20160324 C158C048810300001
BIB 5 13 C048810300002
REACTION (56-BA-134(P,N)57-LA-134,,SGV) C048810300003
ANALYSIS Thermonuclear reaction rates are usually calculated C048810300004
directly from measured reaction cross sections and C048810300005
level parameters. The relevant quantity is NA <sigma C048810300006
v>T which is Avogadro's number times the average C048810300007
value of the product of the cross section times the C048810300008
velocity, averaged over the Maxwell-Boltzmann C048810300009
velocity distribution at the temperature T of interest.C048810300010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048810300011
their values were added quadratically. C048810300012
STATUS (TABLE) Table III, page 193. C048810300013
(DEP,C0488031) C048810300014
HISTORY (20160324C) BP C048810300015
ENDBIB 13 0 C048810300016
NOCOMMON 0 0 C048810300017
DATA 3 10 C048810300018
KT DATA DATA-ERR C048810300019
K9 CM3/S/MOL CM3/S/MOL C048810300020
2.500 2.09E-2 3.14E-3 C048810300021
3.000 7.31E-1 1.10E-1 C048810300022
3.500 9.44E+0 1.42E+0 C048810300023
4.000 6.50E+1 9.75E+0 C048810300024
4.500 2.93E+2 4.40E+1 C048810300025
5.000 9.76E+2 1.92E+2 C048810300026
5.500 2.61E+3 6.73E+2 C048810300027
6.000 5.92E+3 1.91E+3 C048810300028
6.500 1.18E+4 4.61E+3 C048810300029
7.000 2.11E+4 9.75E+3 C048810300030
ENDDATA 12 0 C048810300031
ENDSUBENT 30 0 C048810399999
SUBENT C0488104 20160324 C158C048810400001
BIB 5 13 C048810400002
REACTION (56-BA-136(P,N)57-LA-136,,SGV) C048810400003
ANALYSIS Thermonuclear reaction rates are usually calculated C048810400004
directly from measured reaction cross sections and C048810400005
level parameters. The relevant quantity is NA <sigma C048810400006
v>T which is Avogadro's number times the average C048810400007
value of the product of the cross section times the C048810400008
velocity, averaged over the Maxwell-Boltzmann C048810400009
velocity distribution at the temperature T of interest.C048810400010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048810400011
their values were added quadratically. C048810400012
STATUS (TABLE) Table III, page 193. C048810400013
(DEP,C0488032) C048810400014
HISTORY (20160324C) BP C048810400015
ENDBIB 13 0 C048810400016
NOCOMMON 0 0 C048810400017
DATA 3 12 C048810400018
KT DATA DATA-ERR C048810400019
K9 CM3/S/MOL CM3/S/MOL C048810400020
2.500 2.00E-1 3.00E-2 C048810400021
3.000 3.63E+0 5.44E-1 C048810400022
3.500 3.06E+1 4.59E+0 C048810400023
4.000 1.59E+2 2.39E+1 C048810400024
4.500 5.95E+2 8.93E+1 C048810400025
5.000 1.74E+3 2.61E+2 C048810400026
5.500 4.26E+3 6.73E+2 C048810400027
6.000 9.04E+3 1.89E+3 C048810400028
6.500 1.71E+4 4.53E+3 C048810400029
7.000 2.96E+4 9.59E+3 C048810400030
7.500 4.75E+4 1.82E+4 C048810400031
8.000 7.19E+4 3.21E+4 C048810400032
ENDDATA 14 0 C048810400033
ENDSUBENT 32 0 C048810499999
SUBENT C0488105 20160324 C158C048810500001
BIB 5 13 C048810500002
REACTION (60-ND-143(P,N)61-PM-143,,SGV) C048810500003
ANALYSIS Thermonuclear reaction rates are usually calculated C048810500004
directly from measured reaction cross sections and C048810500005
level parameters. The relevant quantity is NA <sigma C048810500006
v>T which is Avogadro's number times the average C048810500007
value of the product of the cross section times the C048810500008
velocity, averaged over the Maxwell-Boltzmann C048810500009
velocity distribution at the temperature T of interest.C048810500010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048810500011
their values were added quadratically. C048810500012
STATUS (TABLE) Table III, page 193. C048810500013
(DEP,C0488033) C048810500014
HISTORY (20160324C) BP C048810500015
ENDBIB 13 0 C048810500016
NOCOMMON 0 0 C048810500017
DATA 3 8 C048810500018
KT DATA DATA-ERR C048810500019
K9 CM3/S/MOL CM3/S/MOL C048810500020
3.500 1.67E+1 7.87E+0 C048810500021
4.000 1.02E+2 3.85E+1 C048810500022
4.500 4.17E+2 1.42E+2 C048810500023
5.000 1.28E+3 4.44E+2 C048810500024
5.500 3.21E+3 1.22E+3 C048810500025
6.000 6.86E+3 2.94E+3 C048810500026
6.500 1.30E+4 6.36E+3 C048810500027
7.000 2.23E+4 1.24E+4 C048810500028
ENDDATA 10 0 C048810500029
ENDSUBENT 28 0 C048810599999
SUBENT C0488106 20160324 C158C048810600001
BIB 5 13 C048810600002
REACTION (60-ND-144(P,N)61-PM-144,,SGV) C048810600003
ANALYSIS Thermonuclear reaction rates are usually calculated C048810600004
directly from measured reaction cross sections and C048810600005
level parameters. The relevant quantity is NA <sigma C048810600006
v>T which is Avogadro's number times the average C048810600007
value of the product of the cross section times the C048810600008
velocity, averaged over the Maxwell-Boltzmann C048810600009
velocity distribution at the temperature T of interest.C048810600010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048810600011
their values were added quadratically. C048810600012
STATUS (TABLE) Table III, page 193. C048810600013
(DEP,C0488034) C048810600014
HISTORY (20160324C) BP C048810600015
ENDBIB 13 0 C048810600016
NOCOMMON 0 0 C048810600017
DATA 3 8 C048810600018
KT DATA DATA-ERR C048810600019
K9 CM3/S/MOL CM3/S/MOL C048810600020
2.500 1.07E-1 4.44E-2 C048810600021
3.000 1.81E+0 5.26E-1 C048810600022
3.500 1.46E+1 2.72E+0 C048810600023
4.000 7.48E+1 1.12E+1 C048810600024
4.500 2.78E+2 6.20E+1 C048810600025
5.000 8.15E+2 2.48E+2 C048810600026
5.500 2.00E+3 7.99E+2 C048810600027
6.000 4.24E+3 2.13E+3 C048810600028
ENDDATA 10 0 C048810600029
ENDSUBENT 28 0 C048810699999
SUBENT C0488107 20160324 C158C048810700001
BIB 5 13 C048810700002
REACTION (60-ND-146(P,N)61-PM-146,,SGV) C048810700003
ANALYSIS Thermonuclear reaction rates are usually calculated C048810700004
directly from measured reaction cross sections and C048810700005
level parameters. The relevant quantity is NA <sigma C048810700006
v>T which is Avogadro's number times the average C048810700007
value of the product of the cross section times the C048810700008
velocity, averaged over the Maxwell-Boltzmann C048810700009
velocity distribution at the temperature T of interest.C048810700010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048810700011
their values were added quadratically. C048810700012
STATUS (TABLE) Table III, page 193. C048810700013
(DEP,C0488035) C048810700014
HISTORY (20160324C) BP C048810700015
ENDBIB 13 0 C048810700016
NOCOMMON 0 0 C048810700017
DATA 3 8 C048810700018
KT DATA DATA-ERR C048810700019
K9 CM3/S/MOL CM3/S/MOL C048810700020
3.500 4.54E+1 6.81E+0 C048810700021
4.000 2.10E+2 6.47E+1 C048810700022
4.500 7.14E+2 1.79E+2 C048810700023
5.000 1.95E+3 4.82E+2 C048810700024
5.500 4.48E+3 1.26E+3 C048810700025
6.000 9.04E+3 3.07E+3 C048810700026
6.500 1.65E+4 6.76E+3 C048810700027
7.000 2.75E+4 1.34E+4 C048810700028
ENDDATA 10 0 C048810700029
ENDSUBENT 28 0 C048810799999
SUBENT C0488108 20160324 C158C048810800001
BIB 5 13 C048810800002
REACTION (60-ND-148(P,N)61-PM-148,,SGV) C048810800003
ANALYSIS Thermonuclear reaction rates are usually calculated C048810800004
directly from measured reaction cross sections and C048810800005
level parameters. The relevant quantity is NA <sigma C048810800006
v>T which is Avogadro's number times the average C048810800007
value of the product of the cross section times the C048810800008
velocity, averaged over the Maxwell-Boltzmann C048810800009
velocity distribution at the temperature T of interest.C048810800010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048810800011
their values were added quadratically. C048810800012
STATUS (TABLE) Table III, page 194. C048810800013
(DEP,C0488036) C048810800014
HISTORY (20160324C) BP C048810800015
ENDBIB 13 0 C048810800016
NOCOMMON 0 0 C048810800017
DATA 3 9 C048810800018
KT DATA DATA-ERR C048810800019
K9 CM3/S/MOL CM3/S/MOL C048810800020
3.000 1.23E+0 7.12E-1 C048810800021
3.500 9.84E+0 3.39E+0 C048810800022
4.000 4.99E+1 1.23E+1 C048810800023
4.500 1.83E+2 4.24E+1 C048810800024
5.000 5.31E+2 1.44E+2 C048810800025
5.500 1.25E+3 4.33E+2 C048810800026
6.000 2.69E+3 1.12E+3 C048810800027
6.500 5.05E+3 2.53E+3 C048810800028
7.000 8.64E+3 5.45E+3 C048810800029
ENDDATA 11 0 C048810800030
ENDSUBENT 29 0 C048810899999
SUBENT C0488109 20160324 C158C048810900001
BIB 5 13 C048810900002
REACTION (60-ND-148(P,N)61-PM-148-M,,SGV) C048810900003
ANALYSIS Thermonuclear reaction rates are usually calculated C048810900004
directly from measured reaction cross sections and C048810900005
level parameters. The relevant quantity is NA <sigma C048810900006
v>T which is Avogadro's number times the average C048810900007
value of the product of the cross section times the C048810900008
velocity, averaged over the Maxwell-Boltzmann C048810900009
velocity distribution at the temperature T of interest.C048810900010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048810900011
their values were added quadratically. C048810900012
STATUS (TABLE) Table III, page 194. C048810900013
(DEP,C0488037) C048810900014
HISTORY (20160324C) BP C048810900015
ENDBIB 13 0 C048810900016
NOCOMMON 0 0 C048810900017
DATA 3 7 C048810900018
KT DATA DATA-ERR C048810900019
K9 CM3/S/MOL CM3/S/MOL C048810900020
5.000 1.44E+3 1.13E+3 C048810900021
5.500 3.42E+3 2.48E+3 C048810900022
6.000 7.02E+3 4.93E+3 C048810900023
6.500 1.29E+4 9.18E+3 C048810900024
7.000 2.16E+4 1.60E+4 C048810900025
7.500 3.36E+4 2.66E+4 C048810900026
8.000 4.95E+4 4.22E+4 C048810900027
ENDDATA 9 0 C048810900028
ENDSUBENT 27 0 C048810999999
SUBENT C0488110 20160324 C158C048811000001
BIB 5 13 C048811000002
REACTION (60-ND-150(P,N)61-PM-150,,SGV) C048811000003
ANALYSIS Thermonuclear reaction rates are usually calculated C048811000004
directly from measured reaction cross sections and C048811000005
level parameters. The relevant quantity is NA <sigma C048811000006
v>T which is Avogadro's number times the average C048811000007
value of the product of the cross section times the C048811000008
velocity, averaged over the Maxwell-Boltzmann C048811000009
velocity distribution at the temperature T of interest.C048811000010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048811000011
their values were added quadratically. C048811000012
STATUS (TABLE) Table III, page 194. C048811000013
(DEP,C0488038) C048811000014
HISTORY (20160324C) BP C048811000015
ENDBIB 13 0 C048811000016
NOCOMMON 0 0 C048811000017
DATA 3 10 C048811000018
KT DATA DATA-ERR C048811000019
K9 CM3/S/MOL CM3/S/MOL C048811000020
1.500 4.83E-4 1.08E-4 C048811000021
2.000 2.22E-1 3.33E-2 C048811000022
2.500 1.14E+1 1.71E+0 C048811000023
3.000 1.85E+2 2.78E+1 C048811000024
3.500 1.51E+3 2.27E+2 C048811000025
4.000 7.78E+3 1.17E+3 C048811000026
4.500 2.91E+4 5.38E+3 C048811000027
5.000 8.56E+4 2.30E+4 C048811000028
5.500 2.10E+5 7.60E+4 C048811000029
6.000 4.44E+5 2.04E+5 C048811000030
ENDDATA 12 0 C048811000031
ENDSUBENT 30 0 C048811099999
SUBENT C0488111 20160324 C158C048811100001
BIB 5 13 C048811100002
REACTION (62-SM-147(P,N)63-EU-147,,SGV) C048811100003
ANALYSIS Thermonuclear reaction rates are usually calculated C048811100004
directly from measured reaction cross sections and C048811100005
level parameters. The relevant quantity is NA <sigma C048811100006
v>T which is Avogadro's number times the average C048811100007
value of the product of the cross section times the C048811100008
velocity, averaged over the Maxwell-Boltzmann C048811100009
velocity distribution at the temperature T of interest.C048811100010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048811100011
their values were added quadratically. C048811100012
STATUS (TABLE) Table III, page 194. C048811100013
(DEP,C0488039) C048811100014
HISTORY (20160324C) BP C048811100015
ENDBIB 13 0 C048811100016
NOCOMMON 0 0 C048811100017
DATA 3 12 C048811100018
KT DATA DATA-ERR C048811100019
K9 CM3/S/MOL CM3/S/MOL C048811100020
2.500 5.41E-1 1.90E-1 C048811100021
3.000 5.31E+0 1.09E+0 C048811100022
3.500 3.17E+1 4.76E+0 C048811100023
4.000 1.38E+2 2.07E+1 C048811100024
4.500 4.75E+2 7.13E+1 C048811100025
5.000 1.34E+3 2.01E+2 C048811100026
5.500 3.22E+3 4.83E+2 C048811100027
6.000 6.78E+3 1.02E+3 C048811100028
6.500 1.28E+4 1.92E+3 C048811100029
7.000 2.20E+4 3.30E+3 C048811100030
7.500 3.53E+4 5.30E+3 C048811100031
8.000 5.31E+4 7.97E+3 C048811100032
ENDDATA 14 0 C048811100033
ENDSUBENT 32 0 C048811199999
SUBENT C0488112 20160324 C158C048811200001
BIB 5 13 C048811200002
REACTION (62-SM-148(P,N)63-EU-148,,SGV) C048811200003
ANALYSIS Thermonuclear reaction rates are usually calculated C048811200004
directly from measured reaction cross sections and C048811200005
level parameters. The relevant quantity is NA <sigma C048811200006
v>T which is Avogadro's number times the average C048811200007
value of the product of the cross section times the C048811200008
velocity, averaged over the Maxwell-Boltzmann C048811200009
velocity distribution at the temperature T of interest.C048811200010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048811200011
their values were added quadratically. C048811200012
STATUS (TABLE) Table III, page 194. C048811200013
(DEP,C0488040) C048811200014
HISTORY (20160324C) BP C048811200015
ENDBIB 13 0 C048811200016
NOCOMMON 0 0 C048811200017
DATA 3 11 C048811200018
KT DATA DATA-ERR C048811200019
K9 CM3/S/MOL CM3/S/MOL C048811200020
2.500 3.76E-2 5.64E-3 C048811200021
3.000 8.22E-1 1.23E-1 C048811200022
3.500 8.23E+0 1.23E+0 C048811200023
4.000 5.01E+1 7.52E+0 C048811200024
4.500 2.16E+2 3.24E+1 C048811200025
5.000 7.17E+2 1.08E+2 C048811200026
5.500 1.95E+3 3.67E+2 C048811200027
6.000 4.55E+3 1.14E+3 C048811200028
6.500 9.35E+3 2.97E+3 C048811200029
7.000 1.74E+4 6.75E+3 C048811200030
7.500 2.97E+4 1.37E+4 C048811200031
ENDDATA 13 0 C048811200032
ENDSUBENT 31 0 C048811299999
SUBENT C0488113 20160324 C158C048811300001
BIB 5 13 C048811300002
REACTION (62-SM-149(P,N)63-EU-149,,SGV) C048811300003
ANALYSIS Thermonuclear reaction rates are usually calculated C048811300004
directly from measured reaction cross sections and C048811300005
level parameters. The relevant quantity is NA <sigma C048811300006
v>T which is Avogadro's number times the average C048811300007
value of the product of the cross section times the C048811300008
velocity, averaged over the Maxwell-Boltzmann C048811300009
velocity distribution at the temperature T of interest.C048811300010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048811300011
their values were added quadratically. C048811300012
STATUS (TABLE) Table III, page 194. C048811300013
(DEP,C0488041) C048811300014
HISTORY (20160324C) BP C048811300015
ENDBIB 13 0 C048811300016
NOCOMMON 0 0 C048811300017
DATA 3 7 C048811300018
KT DATA DATA-ERR C048811300019
K9 CM3/S/MOL CM3/S/MOL C048811300020
5.000 4.13E+3 2.72E+3 C048811300021
5.500 6.95E+3 3.78E+3 C048811300022
6.000 1.08E+4 5.27E+3 C048811300023
6.500 1.61E+4 6.10E+3 C048811300024
7.000 2.28E+4 7.41E+3 C048811300025
7.500 3.14E+4 9.14E+3 C048811300026
8.000 4.20E+4 1.17E+4 C048811300027
ENDDATA 9 0 C048811300028
ENDSUBENT 27 0 C048811399999
SUBENT C0488114 20160324 C158C048811400001
BIB 5 13 C048811400002
REACTION (62-SM-150(P,N)63-EU-150,,SGV) C048811400003
ANALYSIS Thermonuclear reaction rates are usually calculated C048811400004
directly from measured reaction cross sections and C048811400005
level parameters. The relevant quantity is NA <sigma C048811400006
v>T which is Avogadro's number times the average C048811400007
value of the product of the cross section times the C048811400008
velocity, averaged over the Maxwell-Boltzmann C048811400009
velocity distribution at the temperature T of interest.C048811400010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048811400011
their values were added quadratically. C048811400012
STATUS (TABLE) Table III, page 194. C048811400013
(DEP,C0488042) C048811400014
HISTORY (20160324C) BP C048811400015
ENDBIB 13 0 C048811400016
NOCOMMON 0 0 C048811400017
DATA 3 12 C048811400018
KT DATA DATA-ERR C048811400019
K9 CM3/S/MOL CM3/S/MOL C048811400020
2.500 1.90E-1 2.85E-2 C048811400021
3.000 2.21E+0 3.32E-1 C048811400022
3.500 1.40E+1 2.10E+0 C048811400023
4.000 6.25E+1 9.38E+0 C048811400024
4.500 2.18E+2 3.27E+1 C048811400025
5.000 6.31E+2 9.47E+1 C048811400026
5.500 1.57E+3 2.36E+2 C048811400027
6.000 3.46E+3 7.27E+2 C048811400028
6.500 6.83E+3 1.90E+3 C048811400029
7.000 1.24E+4 4.33E+3 C048811400030
7.500 2.07E+4 8.76E+3 C048811400031
8.000 3.27E+4 1.63E+4 C048811400032
ENDDATA 14 0 C048811400033
ENDSUBENT 32 0 C048811499999
SUBENT C0488115 20160324 C158C048811500001
BIB 5 13 C048811500002
REACTION (62-SM-152(P,N)63-EU-152,,SGV) C048811500003
ANALYSIS Thermonuclear reaction rates are usually calculated C048811500004
directly from measured reaction cross sections and C048811500005
level parameters. The relevant quantity is NA <sigma C048811500006
v>T which is Avogadro's number times the average C048811500007
value of the product of the cross section times the C048811500008
velocity, averaged over the Maxwell-Boltzmann C048811500009
velocity distribution at the temperature T of interest.C048811500010
ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C048811500011
their values were added quadratically. C048811500012
STATUS (TABLE) Table III, page 194. C048811500013
(DEP,C0488043) C048811500014
HISTORY (20160324C) BP C048811500015
ENDBIB 13 0 C048811500016
NOCOMMON 0 0 C048811500017
DATA 3 13 C048811500018
KT DATA DATA-ERR C048811500019
K9 CM3/S/MOL CM3/S/MOL C048811500020
2.000 7.21E-3 2.29E-3 C048811500021
2.500 2.11E-1 3.80E-2 C048811500022
3.000 2.32E+0 3.48E-1 C048811500023
3.500 1.52E+1 2.28E+0 C048811500024
4.000 7.08E+1 1.06E+1 C048811500025
4.500 2.57E+2 3.86E+1 C048811500026
5.000 7.65E+2 1.15E+2 C048811500027
5.500 1.93E+3 2.90E+2 C048811500028
6.000 4.26E+3 7.37E+2 C048811500029
6.500 8.40E+3 1.91E+3 C048811500030
7.000 1.51E+4 4.29E+3 C048811500031
7.500 2.52E+4 8.64E+3 C048811500032
8.000 3.95E+4 1.60E+4 C048811500033
ENDDATA 15 0 C048811500034
ENDSUBENT 33 0 C048811599999
ENDENTRY 115 0 C048899999999