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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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 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