ENTRY C0488 20160321 C158C0488 0 1 SUBENT C0488001 20160321 C158C0488 1 1 BIB 10 24 C0488 1 2 TITLE Thick-target yields and astrophysical thermonuclear C0488 1 3 reaction rates: proton-induced reactions C0488 1 4 AUTHOR (N.A.Roughton,M.J.Fritts,R.J.Peterson,C.S.Zaidins, C0488 1 5 C.J.Hansen) C0488 1 6 REFERENCE (J,AND,23,177,197902) C0488 1 7 #doi:10.1016/0092-640X(79)90004-4 C0488 1 8 REL-REF (O,C0487001,N.A.Roughton+,J,AJ,205,302,1976) Data on C0488 1 9 30 reaction yields that are published in J,AND,23,177, C0488 1 10 197902 and missing in this entry. C0488 1 11 INSTITUTE (1USACLU) C0488 1 12 FACILITY (CYCLO,1USACLU) University of Colorado variable C0488 1 13 energy cyclotron facility. C0488 1 14 SAMPLE Targets were sufficiently thick to stop the beam, and C0488 1 15 assumed to be isotopically pure. C0488 1 16 METHOD (EXTB,SITA,ACTIV) C0488 1 17 DETECTOR (GELI) Ge(Li) detector, shielded by approximately 20 C0488 1 18 cm of lead on all sides to detect beta-delayed decay C0488 1 19 gammas or annihilation quanta. Detector calibration C0488 1 20 results: energy is within 3 keV and efficiency is C0488 1 21 within 5%. C0488 1 22 HISTORY (19990421C) C0488 1 23 (20030625A) Reference corrected, BIB update. C0488 1 24 (20160321A) BP: Updated the entry to the current C0488 1 25 standards, added doi, missing reaction rates data. C0488 1 26 ENDBIB 24 0 C0488 1 27 NOCOMMON 0 0 C0488 1 28 ENDSUBENT 27 0 C0488 199999 SUBENT C0488002 20160321 C158C0488 2 1 BIB 3 10 C0488 2 2 REACTION (7-N-14(P,G)8-O-15,,PY,,TT) C0488 2 3 ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C0488 2 4 . either statistical, due to number of gamma counts, C0488 2 5 . or set to 7% due to uncertainties in of about 5% in C0488 2 6 bombardment parameters such as current integration C0488 2 7 and 5 % in counting due to source location, etc., C0488 2 8 added in quadrature. C0488 2 9 (ERR-1) Bombardment parameters. C0488 2 10 (ERR-2) Source location. C0488 2 11 STATUS (TABLE) Table II, page 184. C0488 2 12 ENDBIB 10 0 C0488 2 13 COMMON 2 3 C0488 2 14 ERR-1 ERR-2 C0488 2 15 PER-CENT PER-CENT C0488 2 16 5.0 5.0 C0488 2 17 ENDCOMMON 3 0 C0488 2 18 DATA 3 13 C0488 2 19 EN-CM DATA DATA-ERR C0488 2 20 MEV PRD/INC PRD/INC C0488 2 21 0.356 3.70E-11 1.90E-11 C0488 2 22 0.665 4.50E-11 9.00E-12 C0488 2 23 0.844 8.50E-11 2.20E-11 C0488 2 24 1.102 8.30E-10 1.20E-10 C0488 2 25 1.282 1.20E-09 4.00E-10 C0488 2 26 1.410 1.50E-09 2.00E-10 C0488 2 27 1.462 1.25E-09 1.30E-10 C0488 2 28 1.550 1.39E-09 1.00E-10 C0488 2 29 1.651 1.67E-09 2.00E-10 C0488 2 30 1.932 3.10E-09 3.00E-10 C0488 2 31 2.226 6.80E-09 5.00E-10 C0488 2 32 2.425 1.20E-08 1.00E-09 C0488 2 33 2.596 1.25E-08 1.50E-09 C0488 2 34 ENDDATA 15 0 C0488 2 35 ENDSUBENT 34 0 C0488 299999 SUBENT C0488003 20160321 C158C0488 3 1 BIB 3 10 C0488 3 2 REACTION (38-SR-87(P,G)39-Y-88,,PY,,TT) C0488 3 3 ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C0488 3 4 . either statistical, due to number of gamma counts, C0488 3 5 . or set to 7% due to uncertainties in of about 5% in C0488 3 6 bombardment parameters such as current integration C0488 3 7 and 5 % in counting due to source location, etc., C0488 3 8 added in quadrature. C0488 3 9 (ERR-1) Bombardment parameters. C0488 3 10 (ERR-2) Source location. C0488 3 11 STATUS (TABLE) Table II, page 185. C0488 3 12 ENDBIB 10 0 C0488 3 13 COMMON 2 3 C0488 3 14 ERR-1 ERR-2 C0488 3 15 PER-CENT PER-CENT C0488 3 16 5.0 5.0 C0488 3 17 ENDCOMMON 3 0 C0488 3 18 DATA 3 7 C0488 3 19 EN-CM DATA DATA-ERR C0488 3 20 MEV PRD/INC PRD/INC C0488 3 21 2.570 4.30E-07 1.40E-07 C0488 3 22 2.780 1.10E-06 3.00E-07 C0488 3 23 2.990 7.30E-07 2.50E-07 C0488 3 24 3.310 1.70E-06 4.00E-07 C0488 3 25 3.350 2.20E-06 4.00E-07 C0488 3 26 3.900 5.00E-06 1.70E-06 C0488 3 27 4.240 9.80E-06 2.40E-06 C0488 3 28 ENDDATA 9 0 C0488 3 29 ENDSUBENT 28 0 C0488 399999 SUBENT C0488004 20160321 C158C0488 4 1 BIB 3 10 C0488 4 2 REACTION (40-ZR-90(P,G)41-NB-91-M,,PY,,TT) C0488 4 3 ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C0488 4 4 . either statistical, due to number of gamma counts, C0488 4 5 . or set to 7% due to uncertainties in of about 5% in C0488 4 6 bombardment parameters such as current integration C0488 4 7 and 5 % in counting due to source location, etc., C0488 4 8 added in quadrature. C0488 4 9 (ERR-1) Bombardment parameters. C0488 4 10 (ERR-2) Source location. C0488 4 11 STATUS (TABLE) Table II, page 185. C0488 4 12 ENDBIB 10 0 C0488 4 13 COMMON 2 3 C0488 4 14 ERR-1 ERR-2 C0488 4 15 PER-CENT PER-CENT C0488 4 16 5.0 5.0 C0488 4 17 ENDCOMMON 3 0 C0488 4 18 DATA 3 15 C0488 4 19 EN-CM DATA DATA-ERR C0488 4 20 MEV PRD/INC PRD/INC C0488 4 21 1.750 3.00E-10 2.00E-10 C0488 4 22 2.047 3.10E-10 2.90E-10 C0488 4 23 2.091 9.00E-10 3.00E-10 C0488 4 24 2.569 3.70E-09 1.00E-09 C0488 4 25 2.786 5.10E-09 8.00E-10 C0488 4 26 3.041 1.72E-08 2.00E-09 C0488 4 27 3.309 3.70E-08 3.00E-09 C0488 4 28 3.770 1.20E-07 1.10E-08 C0488 4 29 4.245 2.65E-07 2.00E-08 C0488 4 30 4.621 5.50E-07 4.00E-08 C0488 4 31 5.180 1.02E-06 8.00E-08 C0488 4 32 5.368 1.45E-06 1.01E-07 C0488 4 33 5.600 2.41E-06 2.00E-07 C0488 4 34 6.015 3.35E-06 2.34E-07 C0488 4 35 6.426 5.30E-06 4.10E-07 C0488 4 36 ENDDATA 17 0 C0488 4 37 ENDSUBENT 36 0 C0488 499999 SUBENT C0488005 20160321 C158C0488 5 1 BIB 3 10 C0488 5 2 REACTION (46-PD-102(P,G)47-AG-103,,PY,,TT) C0488 5 3 ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C0488 5 4 . either statistical, due to number of gamma counts, C0488 5 5 . or set to 7% due to uncertainties in of about 5% in C0488 5 6 bombardment parameters such as current integration C0488 5 7 and 5 % in counting due to source location, etc., C0488 5 8 added in quadrature. C0488 5 9 (ERR-1) Bombardment parameters. C0488 5 10 (ERR-2) Source location. C0488 5 11 STATUS (TABLE) Table II, page 186. C0488 5 12 ENDBIB 10 0 C0488 5 13 COMMON 2 3 C0488 5 14 ERR-1 ERR-2 C0488 5 15 PER-CENT PER-CENT C0488 5 16 5.0 5.0 C0488 5 17 ENDCOMMON 3 0 C0488 5 18 DATA 3 15 C0488 5 19 EN-CM DATA DATA-ERR C0488 5 20 MEV PRD/INC PRD/INC C0488 5 21 2.575 6.54E-10 1.50E-10 C0488 5 22 2.985 5.39E-09 3.77E-10 C0488 5 23 3.483 2.50E-08 1.75E-09 C0488 5 24 3.535 2.15E-08 3.00E-09 C0488 5 25 3.842 7.37E-08 2.00E-08 C0488 5 26 3.976 1.30E-07 9.10E-09 C0488 5 27 4.298 1.31E-07 9.17E-09 C0488 5 28 4.545 3.21E-07 2.25E-08 C0488 5 29 4.652 5.51E-07 3.86E-08 C0488 5 30 4.678 5.29E-07 3.70E-08 C0488 5 31 5.113 7.64E-07 7.60E-08 C0488 5 32 5.223 8.00E-07 4.00E-07 C0488 5 33 5.541 1.53E-06 5.00E-07 C0488 5 34 6.298 4.60E-06 6.09E-06 C0488 5 35 6.770 8.36E-06 1.20E-06 C0488 5 36 ENDDATA 17 0 C0488 5 37 ENDSUBENT 36 0 C0488 599999 SUBENT C0488006 20160321 C158C0488 6 1 BIB 3 10 C0488 6 2 REACTION (48-CD-106(P,G)49-IN-107,,PY,,TT) C0488 6 3 ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C0488 6 4 . either statistical, due to number of gamma counts, C0488 6 5 . or set to 7% due to uncertainties in of about 5% in C0488 6 6 bombardment parameters such as current integration C0488 6 7 and 5 % in counting due to source location, etc., C0488 6 8 added in quadrature. C0488 6 9 (ERR-1) Bombardment parameters. C0488 6 10 (ERR-2) Source location. C0488 6 11 STATUS (TABLE) Table II, page 186. C0488 6 12 ENDBIB 10 0 C0488 6 13 COMMON 2 3 C0488 6 14 ERR-1 ERR-2 C0488 6 15 PER-CENT PER-CENT C0488 6 16 5.0 5.0 C0488 6 17 ENDCOMMON 3 0 C0488 6 18 DATA 3 12 C0488 6 19 EN-CM DATA DATA-ERR C0488 6 20 MEV PRD/INC PRD/INC C0488 6 21 3.000 1.93E-09 3.70E-10 C0488 6 22 3.360 8.74E-09 1.46E-09 C0488 6 23 3.530 9.89E-09 1.71E-09 C0488 6 24 3.830 2.02E-08 2.80E-09 C0488 6 25 3.910 4.91E-08 6.80E-09 C0488 6 26 4.230 5.53E-08 7.40E-09 C0488 6 27 4.350 1.17E-07 1.54E-08 C0488 6 28 4.490 1.25E-07 1.70E-08 C0488 6 29 4.600 2.18E-07 2.90E-08 C0488 6 30 4.660 2.48E-07 3.30E-08 C0488 6 31 4.950 2.92E-07 3.90E-08 C0488 6 32 5.000 4.18E-07 5.50E-08 C0488 6 33 ENDDATA 14 0 C0488 6 34 ENDSUBENT 33 0 C0488 699999 SUBENT C0488007 20160321 C158C0488 7 1 BIB 3 10 C0488 7 2 REACTION (48-CD-108(P,G)49-IN-109,,PY,,TT) C0488 7 3 ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C0488 7 4 . either statistical, due to number of gamma counts, C0488 7 5 . or set to 7% due to uncertainties in of about 5% in C0488 7 6 bombardment parameters such as current integration C0488 7 7 and 5 % in counting due to source location, etc., C0488 7 8 added in quadrature. C0488 7 9 (ERR-1) Bombardment parameters. C0488 7 10 (ERR-2) Source location. C0488 7 11 STATUS (TABLE) Table II, page 186. C0488 7 12 ENDBIB 10 0 C0488 7 13 COMMON 2 3 C0488 7 14 ERR-1 ERR-2 C0488 7 15 PER-CENT PER-CENT C0488 7 16 5.0 5.0 C0488 7 17 ENDCOMMON 3 0 C0488 7 18 DATA 3 12 C0488 7 19 EN-CM DATA DATA-ERR C0488 7 20 MEV PRD/INC PRD/INC C0488 7 21 3.000 4.39E-09 8.30E-10 C0488 7 22 3.360 1.35E-08 2.20E-09 C0488 7 23 3.530 1.31E-08 2.20E-09 C0488 7 24 3.830 5.25E-08 6.90E-09 C0488 7 25 3.910 7.42E-08 9.90E-09 C0488 7 26 4.230 1.23E-07 1.60E-08 C0488 7 27 4.350 1.71E-07 2.20E-08 C0488 7 28 4.490 2.28E-07 3.00E-08 C0488 7 29 4.600 3.69E-07 4.90E-08 C0488 7 30 4.660 3.93E-07 5.10E-08 C0488 7 31 4.950 5.28E-07 6.80E-08 C0488 7 32 5.000 1.06E-06 1.38E-07 C0488 7 33 ENDDATA 14 0 C0488 7 34 ENDSUBENT 33 0 C0488 799999 SUBENT C0488008 20160321 C158C0488 8 1 BIB 3 10 C0488 8 2 REACTION (48-CD-114(P,G)49-IN-115-M,,PY,,TT) C0488 8 3 ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C0488 8 4 . either statistical, due to number of gamma counts, C0488 8 5 . or set to 7% due to uncertainties in of about 5% in C0488 8 6 bombardment parameters such as current integration C0488 8 7 and 5 % in counting due to source location, etc., C0488 8 8 added in quadrature. C0488 8 9 (ERR-1) Bombardment parameters. C0488 8 10 (ERR-2) Source location. C0488 8 11 STATUS (TABLE) Table II, page 186. C0488 8 12 ENDBIB 10 0 C0488 8 13 COMMON 2 3 C0488 8 14 ERR-1 ERR-2 C0488 8 15 PER-CENT PER-CENT C0488 8 16 5.0 5.0 C0488 8 17 ENDCOMMON 3 0 C0488 8 18 DATA 3 13 C0488 8 19 EN-CM DATA DATA-ERR C0488 8 20 MEV PRD/INC PRD/INC C0488 8 21 3.000 8.40E-10 1.20E-10 C0488 8 22 3.060 1.26E-09 1.90E-10 C0488 8 23 3.360 1.98E-09 2.70E-10 C0488 8 24 3.530 2.52E-09 3.40E-10 C0488 8 25 3.830 4.22E-09 4.70E-10 C0488 8 26 3.910 6.28E-09 9.30E-10 C0488 8 27 4.230 6.91E-09 7.70E-10 C0488 8 28 4.350 9.74E-09 1.20E-09 C0488 8 29 4.490 1.18E-08 1.60E-09 C0488 8 30 4.600 1.59E-08 1.90E-09 C0488 8 31 4.660 1.82E-08 2.40E-09 C0488 8 32 4.950 1.99E-08 2.10E-09 C0488 8 33 5.000 3.20E-08 5.70E-09 C0488 8 34 ENDDATA 15 0 C0488 8 35 ENDSUBENT 34 0 C0488 899999 SUBENT C0488009 20160321 C158C0488 9 1 BIB 3 10 C0488 9 2 REACTION (48-CD-116(P,G)49-IN-117-M,,PY,,TT) C0488 9 3 ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C0488 9 4 . either statistical, due to number of gamma counts, C0488 9 5 . or set to 7% due to uncertainties in of about 5% in C0488 9 6 bombardment parameters such as current integration C0488 9 7 and 5 % in counting due to source location, etc., C0488 9 8 added in quadrature. C0488 9 9 (ERR-1) Bombardment parameters. C0488 9 10 (ERR-2) Source location. C0488 9 11 STATUS (TABLE) Table II, page 186. C0488 9 12 ENDBIB 10 0 C0488 9 13 COMMON 2 3 C0488 9 14 ERR-1 ERR-2 C0488 9 15 PER-CENT PER-CENT C0488 9 16 5.0 5.0 C0488 9 17 ENDCOMMON 3 0 C0488 9 18 DATA 3 10 C0488 9 19 EN-CM DATA DATA-ERR C0488 9 20 MEV PRD/INC PRD/INC C0488 9 21 3.000 2.00E-11 2.70E-11 C0488 9 22 3.360 2.04E-10 9.50E-11 C0488 9 23 3.530 1.96E-10 1.07E-10 C0488 9 24 3.830 4.40E-10 1.30E-10 C0488 9 25 3.910 8.10E-10 2.90E-10 C0488 9 26 4.230 9.90E-10 2.30E-10 C0488 9 27 4.350 1.90E-09 7.00E-10 C0488 9 28 4.490 2.30E-09 8.10E-10 C0488 9 29 4.660 4.70E-09 1.10E-09 C0488 9 30 4.950 5.80E-09 2.20E-09 C0488 9 31 ENDDATA 12 0 C0488 9 32 ENDSUBENT 31 0 C0488 999999 SUBENT C0488010 20160321 C158C0488 10 1 BIB 3 10 C0488 10 2 REACTION (50-SN-112(P,G)51-SB-113,,PY,,TT) C0488 10 3 ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C0488 10 4 . either statistical, due to number of gamma counts, C0488 10 5 . or set to 7% due to uncertainties in of about 5% in C0488 10 6 bombardment parameters such as current integration C0488 10 7 and 5 % in counting due to source location, etc., C0488 10 8 added in quadrature. C0488 10 9 (ERR-1) Bombardment parameters. C0488 10 10 (ERR-2) Source location. C0488 10 11 STATUS (TABLE) Table II, page 186. C0488 10 12 ENDBIB 10 0 C0488 10 13 COMMON 2 3 C0488 10 14 ERR-1 ERR-2 C0488 10 15 PER-CENT PER-CENT C0488 10 16 5.0 5.0 C0488 10 17 ENDCOMMON 3 0 C0488 10 18 DATA 3 4 C0488 10 19 EN-CM DATA DATA-ERR C0488 10 20 MEV PRD/INC PRD/INC C0488 10 21 2.987 3.13E-09 4.80E-10 C0488 10 22 3.538 3.25E-08 4.10E-09 C0488 10 23 3.845 7.66E-08 7.00E-09 C0488 10 24 3.979 5.10E-08 2.52E-08 C0488 10 25 ENDDATA 6 0 C0488 10 26 ENDSUBENT 25 0 C0488 1099999 SUBENT C0488011 20160321 C158C0488 11 1 BIB 3 10 C0488 11 2 REACTION (62-SM-144(P,G)63-EU-145,,PY,,TT) C0488 11 3 ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C0488 11 4 . either statistical, due to number of gamma counts, C0488 11 5 . or set to 7% due to uncertainties in of about 5% in C0488 11 6 bombardment parameters such as current integration C0488 11 7 and 5 % in counting due to source location, etc., C0488 11 8 added in quadrature. C0488 11 9 (ERR-1) Bombardment parameters. C0488 11 10 (ERR-2) Source location. C0488 11 11 STATUS (TABLE) Table II, page 186. C0488 11 12 ENDBIB 10 0 C0488 11 13 COMMON 2 3 C0488 11 14 ERR-1 ERR-2 C0488 11 15 PER-CENT PER-CENT C0488 11 16 5.0 5.0 C0488 11 17 ENDCOMMON 3 0 C0488 11 18 DATA 3 11 C0488 11 19 EN-CM DATA DATA-ERR C0488 11 20 MEV PRD/INC PRD/INC C0488 11 21 3.320 1.50E-09 1.50E-09 C0488 11 22 3.379 2.10E-09 5.00E-10 C0488 11 23 3.908 9.25E-09 1.50E-09 C0488 11 24 4.262 1.06E-08 2.90E-09 C0488 11 25 4.616 1.30E-08 2.90E-09 C0488 11 26 5.018 3.28E-08 7.20E-09 C0488 11 27 5.200 4.82E-08 9.60E-09 C0488 11 28 5.389 5.54E-08 7.20E-09 C0488 11 29 5.649 1.49E-07 2.40E-08 C0488 11 30 6.320 6.84E-07 9.60E-08 C0488 11 31 6.792 1.05E-06 1.90E-07 C0488 11 32 ENDDATA 13 0 C0488 11 33 ENDSUBENT 32 0 C0488 1199999 SUBENT C0488012 20160321 C158C0488 12 1 BIB 3 10 C0488 12 2 REACTION (38-SR-87(P,N)39-Y-87,,PY,,TT) C0488 12 3 ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C0488 12 4 . either statistical, due to number of gamma counts, C0488 12 5 . or set to 7% due to uncertainties in of about 5% in C0488 12 6 bombardment parameters such as current integration C0488 12 7 and 5 % in counting due to source location, etc., C0488 12 8 added in quadrature. C0488 12 9 (ERR-1) Bombardment parameters. C0488 12 10 (ERR-2) Source location. C0488 12 11 STATUS (TABLE) Table II, page 187. C0488 12 12 ENDBIB 10 0 C0488 12 13 COMMON 2 3 C0488 12 14 ERR-1 ERR-2 C0488 12 15 PER-CENT PER-CENT C0488 12 16 5.0 5.0 C0488 12 17 ENDCOMMON 3 0 C0488 12 18 DATA 3 12 C0488 12 19 EN-CM DATA DATA-ERR C0488 12 20 MEV PRD/INC PRD/INC C0488 12 21 2.570 1.10E-08 1.00E-09 C0488 12 22 2.780 2.20E-08 2.00E-09 C0488 12 23 2.990 4.60E-08 7.00E-09 C0488 12 24 3.310 5.70E-08 1.60E-08 C0488 12 25 3.350 1.20E-07 1.00E-08 C0488 12 26 3.900 6.40E-07 4.48E-08 C0488 12 27 4.240 1.30E-06 1.00E-07 C0488 12 28 4.590 2.50E-06 5.00E-07 C0488 12 29 4.990 4.00E-06 1.00E-06 C0488 12 30 5.100 7.20E-06 7.00E-07 C0488 12 31 5.180 7.30E-06 1.50E-06 C0488 12 32 5.620 1.30E-05 1.00E-06 C0488 12 33 ENDDATA 14 0 C0488 12 34 ENDSUBENT 33 0 C0488 1299999 SUBENT C0488013 20160321 C158C0488 13 1 BIB 3 10 C0488 13 2 REACTION (38-SR-88(P,N)39-Y-88,,PY,,TT) C0488 13 3 ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C0488 13 4 . either statistical, due to number of gamma counts, C0488 13 5 . or set to 7% due to uncertainties in of about 5% in C0488 13 6 bombardment parameters such as current integration C0488 13 7 and 5 % in counting due to source location, etc., C0488 13 8 added in quadrature. C0488 13 9 (ERR-1) Bombardment parameters. C0488 13 10 (ERR-2) Source location. C0488 13 11 STATUS (TABLE) Table II, page 187. C0488 13 12 ENDBIB 10 0 C0488 13 13 COMMON 2 3 C0488 13 14 ERR-1 ERR-2 C0488 13 15 PER-CENT PER-CENT C0488 13 16 5.0 5.0 C0488 13 17 ENDCOMMON 3 0 C0488 13 18 DATA 3 5 C0488 13 19 EN-CM DATA DATA-ERR C0488 13 20 MEV PRD/INC PRD/INC C0488 13 21 4.590 8.00E-08 7.50E-08 C0488 13 22 4.990 5.20E-06 4.00E-07 C0488 13 23 5.100 9.00E-06 1.00E-06 C0488 13 24 5.180 9.70E-06 1.00E-06 C0488 13 25 5.620 3.90E-05 2.73E-06 C0488 13 26 ENDDATA 7 0 C0488 13 27 ENDSUBENT 26 0 C0488 1399999 SUBENT C0488014 20160321 C158C0488 14 1 BIB 3 10 C0488 14 2 REACTION (40-ZR-94(P,N)41-NB-94-M,,PY,,TT) C0488 14 3 ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C0488 14 4 . either statistical, due to number of gamma counts, C0488 14 5 . or set to 7% due to uncertainties in of about 5% in C0488 14 6 bombardment parameters such as current integration C0488 14 7 and 5 % in counting due to source location, etc., C0488 14 8 added in quadrature. C0488 14 9 (ERR-1) Bombardment parameters. C0488 14 10 (ERR-2) Source location. C0488 14 11 STATUS (TABLE) Table II, page 187. C0488 14 12 ENDBIB 10 0 C0488 14 13 COMMON 2 3 C0488 14 14 ERR-1 ERR-2 C0488 14 15 PER-CENT PER-CENT C0488 14 16 5.0 5.0 C0488 14 17 ENDCOMMON 3 0 C0488 14 18 DATA 3 13 C0488 14 19 EN-CM DATA DATA-ERR C0488 14 20 MEV PRD/INC PRD/INC C0488 14 21 3.056 1.67E-07 1.67E-08 C0488 14 22 3.480 6.73E-07 6.73E-08 C0488 14 23 3.530 8.24E-07 8.24E-08 C0488 14 24 3.840 2.14E-06 2.14E-07 C0488 14 25 3.972 2.62E-06 2.62E-07 C0488 14 26 4.294 3.98E-06 3.98E-07 C0488 14 27 4.640 7.89E-06 7.89E-07 C0488 14 28 4.716 1.51E-05 1.51E-06 C0488 14 29 4.720 1.51E-05 1.51E-06 C0488 14 30 4.942 1.89E-05 1.89E-06 C0488 14 31 5.220 3.31E-05 3.31E-06 C0488 14 32 5.536 5.82E-05 5.82E-06 C0488 14 33 5.953 7.42E-05 7.42E-06 C0488 14 34 ENDDATA 15 0 C0488 14 35 ENDSUBENT 34 0 C0488 1499999 SUBENT C0488015 20160321 C158C0488 15 1 BIB 3 10 C0488 15 2 REACTION (40-ZR-96(P,N)41-NB-96,,PY,,TT) C0488 15 3 ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C0488 15 4 . either statistical, due to number of gamma counts, C0488 15 5 . or set to 7% due to uncertainties in of about 5% in C0488 15 6 bombardment parameters such as current integration C0488 15 7 and 5 % in counting due to source location, etc., C0488 15 8 added in quadrature. C0488 15 9 (ERR-1) Bombardment parameters. C0488 15 10 (ERR-2) Source location. C0488 15 11 STATUS (TABLE) Table II, page 187. C0488 15 12 ENDBIB 10 0 C0488 15 13 COMMON 2 3 C0488 15 14 ERR-1 ERR-2 C0488 15 15 PER-CENT PER-CENT C0488 15 16 5.0 5.0 C0488 15 17 ENDCOMMON 3 0 C0488 15 18 DATA 3 12 C0488 15 19 EN-CM DATA DATA-ERR C0488 15 20 MEV PRD/INC PRD/INC C0488 15 21 3.057 4.48E-08 4.48E-09 C0488 15 22 3.480 2.35E-07 2.35E-08 C0488 15 23 3.530 2.71E-07 2.71E-08 C0488 15 24 3.840 5.37E-07 5.37E-08 C0488 15 25 3.974 1.01E-06 1.01E-07 C0488 15 26 4.295 1.88E-06 1.88E-07 C0488 15 27 4.640 3.53E-06 3.53E-07 C0488 15 28 4.720 4.54E-06 4.54E-07 C0488 15 29 4.945 6.80E-06 6.80E-07 C0488 15 30 5.220 1.42E-05 1.42E-06 C0488 15 31 5.537 2.26E-05 2.26E-06 C0488 15 32 5.954 3.69E-05 3.69E-06 C0488 15 33 ENDDATA 14 0 C0488 15 34 ENDSUBENT 33 0 C0488 1599999 SUBENT C0488016 20160321 C158C0488 16 1 BIB 3 10 C0488 16 2 REACTION (46-PD-104(P,N)47-AG-104,,PY,,TT) C0488 16 3 ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C0488 16 4 . either statistical, due to number of gamma counts, C0488 16 5 . or set to 7% due to uncertainties in of about 5% in C0488 16 6 bombardment parameters such as current integration C0488 16 7 and 5 % in counting due to source location, etc., C0488 16 8 added in quadrature. C0488 16 9 (ERR-1) Bombardment parameters. C0488 16 10 (ERR-2) Source location. C0488 16 11 STATUS (TABLE) Table II, page 187. C0488 16 12 ENDBIB 10 0 C0488 16 13 COMMON 2 3 C0488 16 14 ERR-1 ERR-2 C0488 16 15 PER-CENT PER-CENT C0488 16 16 5.0 5.0 C0488 16 17 ENDCOMMON 3 0 C0488 16 18 DATA 3 4 C0488 16 19 EN-CM DATA DATA-ERR C0488 16 20 MEV PRD/INC PRD/INC C0488 16 21 5.118 6.90E-09 1.08E-09 C0488 16 22 5.225 2.75E-07 4.13E-08 C0488 16 23 5.542 8.34E-07 5.84E-08 C0488 16 24 5.958 4.46E-06 6.69E-07 C0488 16 25 ENDDATA 6 0 C0488 16 26 ENDSUBENT 25 0 C0488 1699999 SUBENT C0488017 20160321 C158C0488 17 1 BIB 3 10 C0488 17 2 REACTION (46-PD-105(P,N)47-AG-105,,PY,,TT) C0488 17 3 ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C0488 17 4 . either statistical, due to number of gamma counts, C0488 17 5 . or set to 7% due to uncertainties in of about 5% in C0488 17 6 bombardment parameters such as current integration C0488 17 7 and 5 % in counting due to source location, etc., C0488 17 8 added in quadrature. C0488 17 9 (ERR-1) Bombardment parameters. C0488 17 10 (ERR-2) Source location. C0488 17 11 STATUS (TABLE) Table II, page 187. C0488 17 12 ENDBIB 10 0 C0488 17 13 COMMON 2 3 C0488 17 14 ERR-1 ERR-2 C0488 17 15 PER-CENT PER-CENT C0488 17 16 5.0 5.0 C0488 17 17 ENDCOMMON 3 0 C0488 17 18 DATA 3 11 C0488 17 19 EN-CM DATA DATA-ERR C0488 17 20 MEV PRD/INC PRD/INC C0488 17 21 3.536 5.09E-08 7.63E-09 C0488 17 22 3.843 1.32E-07 1.98E-08 C0488 17 23 3.980 2.56E-07 6.00E-08 C0488 17 24 4.300 5.72E-07 8.58E-08 C0488 17 25 4.547 1.26E-06 1.26E-07 C0488 17 26 4.679 1.68E-06 1.68E-07 C0488 17 27 4.954 2.33E-06 2.33E-07 C0488 17 28 5.114 4.20E-06 4.20E-07 C0488 17 29 5.225 4.62E-06 4.62E-07 C0488 17 30 5.542 8.49E-06 8.49E-07 C0488 17 31 5.960 1.36E-05 1.36E-06 C0488 17 32 ENDDATA 13 0 C0488 17 33 ENDSUBENT 32 0 C0488 1799999 SUBENT C0488018 20160321 C158C0488 18 1 BIB 3 10 C0488 18 2 REACTION (46-PD-106(P,N)47-AG-106,,PY,,TT) C0488 18 3 ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C0488 18 4 . either statistical, due to number of gamma counts, C0488 18 5 . or set to 7% due to uncertainties in of about 5% in C0488 18 6 bombardment parameters such as current integration C0488 18 7 and 5 % in counting due to source location, etc., C0488 18 8 added in quadrature. C0488 18 9 (ERR-1) Bombardment parameters. C0488 18 10 (ERR-2) Source location. C0488 18 11 STATUS (TABLE) Table II, page 187. C0488 18 12 ENDBIB 10 0 C0488 18 13 COMMON 2 3 C0488 18 14 ERR-1 ERR-2 C0488 18 15 PER-CENT PER-CENT C0488 18 16 5.0 5.0 C0488 18 17 ENDCOMMON 3 0 C0488 18 18 DATA 3 7 C0488 18 19 EN-CM DATA DATA-ERR C0488 18 20 MEV PRD/INC PRD/INC C0488 18 21 3.977 1.74E-07 2.61E-08 C0488 18 22 4.299 6.14E-07 9.21E-08 C0488 18 23 4.547 3.48E-06 5.43E-07 C0488 18 24 4.954 6.47E-06 9.70E-07 C0488 18 25 5.226 9.83E-06 1.95E-06 C0488 18 26 5.543 2.93E-05 5.10E-06 C0488 18 27 5.960 5.14E-05 5.40E-06 C0488 18 28 ENDDATA 9 0 C0488 18 29 ENDSUBENT 28 0 C0488 1899999 SUBENT C0488019 20160321 C158C0488 19 1 BIB 3 10 C0488 19 2 REACTION (46-PD-106(P,N)47-AG-106-M,,PY,,TT) C0488 19 3 ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C0488 19 4 . either statistical, due to number of gamma counts, C0488 19 5 . or set to 7% due to uncertainties in of about 5% in C0488 19 6 bombardment parameters such as current integration C0488 19 7 and 5 % in counting due to source location, etc., C0488 19 8 added in quadrature. C0488 19 9 (ERR-1) Bombardment parameters. C0488 19 10 (ERR-2) Source location. C0488 19 11 STATUS (TABLE) Table II, page 187. C0488 19 12 ENDBIB 10 0 C0488 19 13 COMMON 2 3 C0488 19 14 ERR-1 ERR-2 C0488 19 15 PER-CENT PER-CENT C0488 19 16 5.0 5.0 C0488 19 17 ENDCOMMON 3 0 C0488 19 18 DATA 3 8 C0488 19 19 EN-CM DATA DATA-ERR C0488 19 20 MEV PRD/INC PRD/INC C0488 19 21 3.977 6.90E-10 6.20E-10 C0488 19 22 4.547 4.27E-08 6.40E-09 C0488 19 23 4.679 2.20E-08 7.50E-09 C0488 19 24 4.954 3.64E-08 1.25E-08 C0488 19 25 5.114 1.29E-07 2.50E-08 C0488 19 26 5.225 7.90E-08 1.25E-08 C0488 19 27 5.543 1.32E-07 1.88E-08 C0488 19 28 5.959 4.02E-07 6.03E-08 C0488 19 29 ENDDATA 10 0 C0488 19 30 ENDSUBENT 29 0 C0488 1999999 SUBENT C0488020 20160321 C158C0488 20 1 BIB 3 10 C0488 20 2 REACTION (48-CD-116(P,N)49-IN-116-M,,PY,,TT) C0488 20 3 ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C0488 20 4 . either statistical, due to number of gamma counts, C0488 20 5 . or set to 7% due to uncertainties in of about 5% in C0488 20 6 bombardment parameters such as current integration C0488 20 7 and 5 % in counting due to source location, etc., C0488 20 8 added in quadrature. C0488 20 9 (ERR-1) Bombardment parameters. C0488 20 10 (ERR-2) Source location. C0488 20 11 STATUS (TABLE) Table II, page 187. C0488 20 12 ENDBIB 10 0 C0488 20 13 COMMON 2 3 C0488 20 14 ERR-1 ERR-2 C0488 20 15 PER-CENT PER-CENT C0488 20 16 5.0 5.0 C0488 20 17 ENDCOMMON 3 0 C0488 20 18 DATA 3 12 C0488 20 19 EN-CM DATA DATA-ERR C0488 20 20 MEV PRD/INC PRD/INC C0488 20 21 3.000 8.23E-10 2.34E-10 C0488 20 22 3.360 5.05E-09 9.40E-10 C0488 20 23 3.530 5.91E-09 9.90E-10 C0488 20 24 3.830 2.05E-08 3.00E-09 C0488 20 25 3.910 3.65E-08 5.50E-09 C0488 20 26 4.230 6.48E-08 9.50E-09 C0488 20 27 4.350 1.18E-07 1.70E-08 C0488 20 28 4.490 1.47E-07 2.10E-08 C0488 20 29 4.610 2.60E-07 3.80E-08 C0488 20 30 4.660 2.99E-07 5.70E-08 C0488 20 31 4.950 4.28E-07 6.20E-08 C0488 20 32 5.000 8.43E-07 1.32E-07 C0488 20 33 ENDDATA 14 0 C0488 20 34 ENDSUBENT 33 0 C0488 2099999 SUBENT C0488021 20160321 C158C0488 21 1 BIB 3 10 C0488 21 2 REACTION (50-SN-115(P,N)51-SB-115,,PY,,TT) C0488 21 3 ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C0488 21 4 . either statistical, due to number of gamma counts, C0488 21 5 . or set to 7% due to uncertainties in of about 5% in C0488 21 6 bombardment parameters such as current integration C0488 21 7 and 5 % in counting due to source location, etc., C0488 21 8 added in quadrature. C0488 21 9 (ERR-1) Bombardment parameters. C0488 21 10 (ERR-2) Source location. C0488 21 11 STATUS (TABLE) Table II, page 187. C0488 21 12 ENDBIB 10 0 C0488 21 13 COMMON 2 3 C0488 21 14 ERR-1 ERR-2 C0488 21 15 PER-CENT PER-CENT C0488 21 16 5.0 5.0 C0488 21 17 ENDCOMMON 3 0 C0488 21 18 DATA 3 4 C0488 21 19 EN-CM DATA DATA-ERR C0488 21 20 MEV PRD/INC PRD/INC C0488 21 21 4.683 2.42E-07 3.40E-08 C0488 21 22 5.118 1.35E-06 2.00E-07 C0488 21 23 5.547 2.80E-06 4.20E-07 C0488 21 24 5.964 1.12E-05 1.68E-06 C0488 21 25 ENDDATA 6 0 C0488 21 26 ENDSUBENT 25 0 C0488 2199999 SUBENT C0488022 20160321 C158C0488 22 1 BIB 3 10 C0488 22 2 REACTION (50-SN-117(P,N)51-SB-117,,PY,,TT) C0488 22 3 ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C0488 22 4 . either statistical, due to number of gamma counts, C0488 22 5 . or set to 7% due to uncertainties in of about 5% in C0488 22 6 bombardment parameters such as current integration C0488 22 7 and 5 % in counting due to source location, etc., C0488 22 8 added in quadrature. C0488 22 9 (ERR-1) Bombardment parameters. C0488 22 10 (ERR-2) Source location. C0488 22 11 STATUS (TABLE) Table II, page 187. C0488 22 12 ENDBIB 10 0 C0488 22 13 COMMON 2 3 C0488 22 14 ERR-1 ERR-2 C0488 22 15 PER-CENT PER-CENT C0488 22 16 5.0 5.0 C0488 22 17 ENDCOMMON 3 0 C0488 22 18 DATA 3 11 C0488 22 19 EN-CM DATA DATA-ERR C0488 22 20 MEV PRD/INC PRD/INC C0488 22 21 2.988 4.34E-09 6.51E-10 C0488 22 22 3.539 3.01E-08 4.50E-09 C0488 22 23 3.847 8.20E-08 1.23E-08 C0488 22 24 4.302 3.01E-07 4.50E-08 C0488 22 25 4.551 9.80E-07 1.47E-07 C0488 22 26 4.683 1.50E-06 2.25E-07 C0488 22 27 4.958 1.72E-06 2.58E-07 C0488 22 28 5.119 3.78E-06 5.67E-07 C0488 22 29 5.230 4.58E-06 6.87E-07 C0488 22 30 5.547 7.27E-06 1.09E-06 C0488 22 31 5.965 1.45E-05 2.18E-06 C0488 22 32 ENDDATA 13 0 C0488 22 33 ENDSUBENT 32 0 C0488 2299999 SUBENT C0488023 20160321 C158C0488 23 1 BIB 3 10 C0488 23 2 REACTION (50-SN-120(P,N)51-SB-120,,PY,,TT) C0488 23 3 ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C0488 23 4 . either statistical, due to number of gamma counts, C0488 23 5 . or set to 7% due to uncertainties in of about 5% in C0488 23 6 bombardment parameters such as current integration C0488 23 7 and 5 % in counting due to source location, etc., C0488 23 8 added in quadrature. C0488 23 9 (ERR-1) Bombardment parameters. C0488 23 10 (ERR-2) Source location. C0488 23 11 STATUS (TABLE) Table II, page 188. C0488 23 12 ENDBIB 10 0 C0488 23 13 COMMON 2 3 C0488 23 14 ERR-1 ERR-2 C0488 23 15 PER-CENT PER-CENT C0488 23 16 5.0 5.0 C0488 23 17 ENDCOMMON 3 0 C0488 23 18 DATA 3 9 C0488 23 19 EN-CM DATA DATA-ERR C0488 23 20 MEV PRD/INC PRD/INC C0488 23 21 3.540 7.00E-09 1.05E-09 C0488 23 22 3.848 3.89E-08 5.83E-09 C0488 23 23 3.982 8.67E-08 1.30E-08 C0488 23 24 4.304 1.57E-07 2.30E-08 C0488 23 25 4.552 5.75E-07 8.63E-08 C0488 23 26 4.685 9.66E-07 6.76E-08 C0488 23 27 5.120 2.53E-06 3.79E-07 C0488 23 28 5.548 4.69E-06 7.04E-07 C0488 23 29 5.966 1.03E-05 1.55E-06 C0488 23 30 ENDDATA 11 0 C0488 23 31 ENDSUBENT 30 0 C0488 2399999 SUBENT C0488024 20160321 C158C0488 24 1 BIB 3 10 C0488 24 2 REACTION (50-SN-122(P,N)51-SB-122,,PY,,TT) C0488 24 3 ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C0488 24 4 . either statistical, due to number of gamma counts, C0488 24 5 . or set to 7% due to uncertainties in of about 5% in C0488 24 6 bombardment parameters such as current integration C0488 24 7 and 5 % in counting due to source location, etc., C0488 24 8 added in quadrature. C0488 24 9 (ERR-1) Bombardment parameters. C0488 24 10 (ERR-2) Source location. C0488 24 11 STATUS (TABLE) Table II, page 188. C0488 24 12 ENDBIB 10 0 C0488 24 13 COMMON 2 3 C0488 24 14 ERR-1 ERR-2 C0488 24 15 PER-CENT PER-CENT C0488 24 16 5.0 5.0 C0488 24 17 ENDCOMMON 3 0 C0488 24 18 DATA 3 8 C0488 24 19 EN-CM DATA DATA-ERR C0488 24 20 MEV PRD/INC PRD/INC C0488 24 21 3.850 7.77E-08 1.79E+00 C0488 24 22 3.980 1.38E-07 2.09E+00 C0488 24 23 4.300 1.79E-07 2.09E+00 C0488 24 24 4.550 6.43E-07 5.97E+00 C0488 24 25 4.960 1.17E-06 1.19E+00 C0488 24 26 5.230 2.72E-06 7.47E+00 C0488 24 27 5.550 5.08E-06 3.59E+00 C0488 24 28 5.970 1.09E-05 7.47E+00 C0488 24 29 ENDDATA 10 0 C0488 24 30 ENDSUBENT 29 0 C0488 2499999 SUBENT C0488025 20160321 C158C0488 25 1 BIB 3 10 C0488 25 2 REACTION (50-SN-124(P,N)51-SB-124,,PY,,TT) C0488 25 3 ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C0488 25 4 . either statistical, due to number of gamma counts, C0488 25 5 . or set to 7% due to uncertainties in of about 5% in C0488 25 6 bombardment parameters such as current integration C0488 25 7 and 5 % in counting due to source location, etc., C0488 25 8 added in quadrature. C0488 25 9 (ERR-1) Bombardment parameters. C0488 25 10 (ERR-2) Source location. C0488 25 11 STATUS (TABLE) Table II, page 188. C0488 25 12 ENDBIB 10 0 C0488 25 13 COMMON 2 3 C0488 25 14 ERR-1 ERR-2 C0488 25 15 PER-CENT PER-CENT C0488 25 16 5.0 5.0 C0488 25 17 ENDCOMMON 3 0 C0488 25 18 DATA 3 9 C0488 25 19 EN-CM DATA DATA-ERR C0488 25 20 MEV PRD/INC PRD/INC C0488 25 21 3.983 1.19E-07 6.20E-08 C0488 25 22 4.305 2.68E-07 1.40E-07 C0488 25 23 4.550 1.10E-06 3.50E-07 C0488 25 24 4.686 1.33E-06 2.00E-07 C0488 25 25 4.961 1.37E-06 2.06E-07 C0488 25 26 5.122 1.84E-06 2.76E-07 C0488 25 27 5.233 3.07E-06 5.27E-07 C0488 25 28 5.550 8.25E-06 1.23E-06 C0488 25 29 5.967 1.09E-05 1.64E-06 C0488 25 30 ENDDATA 11 0 C0488 25 31 ENDSUBENT 30 0 C0488 2599999 SUBENT C0488026 20160321 C158C0488 26 1 BIB 3 10 C0488 26 2 REACTION (52-TE-123(P,N)53-I-123,,PY,,TT) C0488 26 3 ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C0488 26 4 . either statistical, due to number of gamma counts, C0488 26 5 . or set to 7% due to uncertainties in of about 5% in C0488 26 6 bombardment parameters such as current integration C0488 26 7 and 5 % in counting due to source location, etc., C0488 26 8 added in quadrature. C0488 26 9 (ERR-1) Bombardment parameters. C0488 26 10 (ERR-2) Source location. C0488 26 11 STATUS (TABLE) Table II, page 188. C0488 26 12 ENDBIB 10 0 C0488 26 13 COMMON 2 3 C0488 26 14 ERR-1 ERR-2 C0488 26 15 PER-CENT PER-CENT C0488 26 16 5.0 5.0 C0488 26 17 ENDCOMMON 3 0 C0488 26 18 DATA 3 10 C0488 26 19 EN-CM DATA DATA-ERR C0488 26 20 MEV PRD/INC PRD/INC C0488 26 21 3.050 1.30E-09 9.00E-10 C0488 26 22 3.317 1.80E-08 9.00E-10 C0488 26 23 3.373 1.10E-08 4.00E-10 C0488 26 24 3.902 2.00E-07 3.00E-08 C0488 26 25 4.257 3.00E-07 3.00E-08 C0488 26 26 4.607 1.40E-06 1.00E-08 C0488 26 27 5.008 3.60E-06 3.00E-07 C0488 26 28 5.641 9.40E-06 7.00E-07 C0488 26 29 6.033 1.20E-05 1.00E-07 C0488 26 30 6.308 1.60E-05 2.00E-06 C0488 26 31 ENDDATA 12 0 C0488 26 32 ENDSUBENT 31 0 C0488 2699999 SUBENT C0488027 20160321 C158C0488 27 1 BIB 3 10 C0488 27 2 REACTION (52-TE-126(P,N)53-I-126,,PY,,TT) C0488 27 3 ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C0488 27 4 . either statistical, due to number of gamma counts, C0488 27 5 . or set to 7% due to uncertainties in of about 5% in C0488 27 6 bombardment parameters such as current integration C0488 27 7 and 5 % in counting due to source location, etc., C0488 27 8 added in quadrature. C0488 27 9 (ERR-1) Bombardment parameters. C0488 27 10 (ERR-2) Source location. C0488 27 11 STATUS (TABLE) Table II, page 188. C0488 27 12 ENDBIB 10 0 C0488 27 13 COMMON 2 3 C0488 27 14 ERR-1 ERR-2 C0488 27 15 PER-CENT PER-CENT C0488 27 16 5.0 5.0 C0488 27 17 ENDCOMMON 3 0 C0488 27 18 DATA 3 10 C0488 27 19 EN-CM DATA DATA-ERR C0488 27 20 MEV PRD/INC PRD/INC C0488 27 21 3.005 3.40E-09 8.00E-10 C0488 27 22 3.320 4.50E-09 3.15E-10 C0488 27 23 3.374 8.10E-09 5.67E-10 C0488 27 24 3.903 6.20E-08 1.30E-08 C0488 27 25 4.258 1.10E-07 3.00E-08 C0488 27 26 4.608 5.30E-07 3.71E-08 C0488 27 27 5.009 1.60E-06 2.00E-07 C0488 27 28 5.642 3.80E-06 3.00E-07 C0488 27 29 6.034 6.30E-06 5.00E-07 C0488 27 30 6.310 1.10E-05 1.00E-06 C0488 27 31 ENDDATA 12 0 C0488 27 32 ENDSUBENT 31 0 C0488 2799999 SUBENT C0488028 20160321 C158C0488 28 1 BIB 3 10 C0488 28 2 REACTION (52-TE-128(P,N)53-I-128,,PY,,TT) C0488 28 3 ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C0488 28 4 . either statistical, due to number of gamma counts, C0488 28 5 . or set to 7% due to uncertainties in of about 5% in C0488 28 6 bombardment parameters such as current integration C0488 28 7 and 5 % in counting due to source location, etc., C0488 28 8 added in quadrature. C0488 28 9 (ERR-1) Bombardment parameters. C0488 28 10 (ERR-2) Source location. C0488 28 11 STATUS (TABLE) Table II, page 188. C0488 28 12 ENDBIB 10 0 C0488 28 13 COMMON 2 3 C0488 28 14 ERR-1 ERR-2 C0488 28 15 PER-CENT PER-CENT C0488 28 16 5.0 5.0 C0488 28 17 ENDCOMMON 3 0 C0488 28 18 DATA 3 11 C0488 28 19 EN-CM DATA DATA-ERR C0488 28 20 MEV PRD/INC PRD/INC C0488 28 21 2.795 5.30E-10 2.80E-10 C0488 28 22 3.005 7.20E-10 9.00E-11 C0488 28 23 3.051 6.80E-10 1.90E-10 C0488 28 24 3.320 4.70E-09 3.29E-10 C0488 28 25 3.903 4.10E-08 2.87E-09 C0488 28 26 4.259 9.10E-08 6.37E-09 C0488 28 27 4.609 3.00E-07 3.00E-08 C0488 28 28 5.010 7.90E-07 6.00E-08 C0488 28 29 5.643 2.60E-06 2.00E-07 C0488 28 30 6.035 5.00E-06 3.50E-07 C0488 28 31 6.310 5.80E-06 4.06E-07 C0488 28 32 ENDDATA 13 0 C0488 28 33 ENDSUBENT 32 0 C0488 2899999 SUBENT C0488029 20160321 C158C0488 29 1 BIB 3 10 C0488 29 2 REACTION (52-TE-130(P,N)53-I-130,,PY,,TT) C0488 29 3 ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C0488 29 4 . either statistical, due to number of gamma counts, C0488 29 5 . or set to 7% due to uncertainties in of about 5% in C0488 29 6 bombardment parameters such as current integration C0488 29 7 and 5 % in counting due to source location, etc., C0488 29 8 added in quadrature. C0488 29 9 (ERR-1) Bombardment parameters. C0488 29 10 (ERR-2) Source location. C0488 29 11 STATUS (TABLE) Table II, page 188. C0488 29 12 ENDBIB 10 0 C0488 29 13 COMMON 2 3 C0488 29 14 ERR-1 ERR-2 C0488 29 15 PER-CENT PER-CENT C0488 29 16 5.0 5.0 C0488 29 17 ENDCOMMON 3 0 C0488 29 18 DATA 3 12 C0488 29 19 EN-CM DATA DATA-ERR C0488 29 20 MEV PRD/INC PRD/INC C0488 29 21 2.796 7.00E-10 6.00E-10 C0488 29 22 3.006 1.80E-09 3.00E-10 C0488 29 23 3.052 1.10E-09 3.00E-10 C0488 29 24 3.321 4.90E-09 9.00E-10 C0488 29 25 3.375 3.40E-09 6.00E-10 C0488 29 26 3.904 5.50E-08 3.85E-09 C0488 29 27 4.259 1.10E-07 1.00E-08 C0488 29 28 4.610 3.80E-07 2.66E-08 C0488 29 29 5.011 1.10E-06 1.00E-07 C0488 29 30 5.644 3.60E-06 2.52E-07 C0488 29 31 6.036 4.90E-06 9.00E-07 C0488 29 32 6.312 9.50E-06 6.65E-07 C0488 29 33 ENDDATA 14 0 C0488 29 34 ENDSUBENT 33 0 C0488 2999999 SUBENT C0488030 20160321 C158C0488 30 1 BIB 3 10 C0488 30 2 REACTION (52-TE-130(P,N)53-I-130-M,,PY,,TT) C0488 30 3 ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C0488 30 4 . either statistical, due to number of gamma counts, C0488 30 5 . or set to 7% due to uncertainties in of about 5% in C0488 30 6 bombardment parameters such as current integration C0488 30 7 and 5 % in counting due to source location, etc., C0488 30 8 added in quadrature. C0488 30 9 (ERR-1) Bombardment parameters. C0488 30 10 (ERR-2) Source location. C0488 30 11 STATUS (TABLE) Table II, page 188. C0488 30 12 ENDBIB 10 0 C0488 30 13 COMMON 2 3 C0488 30 14 ERR-1 ERR-2 C0488 30 15 PER-CENT PER-CENT C0488 30 16 5.0 5.0 C0488 30 17 ENDCOMMON 3 0 C0488 30 18 DATA 3 8 C0488 30 19 EN-CM DATA DATA-ERR C0488 30 20 MEV PRD/INC PRD/INC C0488 30 21 2.796 1.30E-09 5.00E-10 C0488 30 22 3.052 4.90E-09 7.00E-10 C0488 30 23 3.321 2.30E-08 7.00E-09 C0488 30 24 4.259 1.80E-07 7.00E-08 C0488 30 25 4.610 2.10E-07 2.00E-08 C0488 30 26 5.011 6.80E-07 9.00E-08 C0488 30 27 5.644 1.70E-06 2.00E-07 C0488 30 28 6.312 4.40E-06 5.00E-07 C0488 30 29 ENDDATA 10 0 C0488 30 30 ENDSUBENT 29 0 C0488 3099999 SUBENT C0488031 20160321 C158C0488 31 1 BIB 3 10 C0488 31 2 REACTION (56-BA-134(P,N)57-LA-134,,PY,,TT) C0488 31 3 ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C0488 31 4 . either statistical, due to number of gamma counts, C0488 31 5 . or set to 7% due to uncertainties in of about 5% in C0488 31 6 bombardment parameters such as current integration C0488 31 7 and 5 % in counting due to source location, etc., C0488 31 8 added in quadrature. C0488 31 9 (ERR-1) Bombardment parameters. C0488 31 10 (ERR-2) Source location. C0488 31 11 STATUS (TABLE) Table II, page 188. C0488 31 12 ENDBIB 10 0 C0488 31 13 COMMON 2 3 C0488 31 14 ERR-1 ERR-2 C0488 31 15 PER-CENT PER-CENT C0488 31 16 5.0 5.0 C0488 31 17 ENDCOMMON 3 0 C0488 31 18 DATA 3 7 C0488 31 19 EN-CM DATA DATA-ERR C0488 31 20 MEV PRD/INC PRD/INC C0488 31 21 4.611 2.30E-08 6.00E-09 C0488 31 22 5.008 2.00E-07 2.00E-08 C0488 31 23 5.125 2.70E-07 2.00E-08 C0488 31 24 5.388 6.00E-07 5.00E-08 C0488 31 25 5.642 8.40E-07 8.00E-08 C0488 31 26 6.037 2.60E-06 3.00E-07 C0488 31 27 6.315 3.00E-06 3.00E-07 C0488 31 28 ENDDATA 9 0 C0488 31 29 ENDSUBENT 28 0 C0488 3199999 SUBENT C0488032 20160321 C158C0488 32 1 BIB 3 10 C0488 32 2 REACTION (56-BA-136(P,N)57-LA-136,,PY,,TT) C0488 32 3 ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C0488 32 4 . either statistical, due to number of gamma counts, C0488 32 5 . or set to 7% due to uncertainties in of about 5% in C0488 32 6 bombardment parameters such as current integration C0488 32 7 and 5 % in counting due to source location, etc., C0488 32 8 added in quadrature. C0488 32 9 (ERR-1) Bombardment parameters. C0488 32 10 (ERR-2) Source location. C0488 32 11 STATUS (TABLE) Table II, page 188. C0488 32 12 ENDBIB 10 0 C0488 32 13 COMMON 2 3 C0488 32 14 ERR-1 ERR-2 C0488 32 15 PER-CENT PER-CENT C0488 32 16 5.0 5.0 C0488 32 17 ENDCOMMON 3 0 C0488 32 18 DATA 3 9 C0488 32 19 EN-CM DATA DATA-ERR C0488 32 20 MEV PRD/INC PRD/INC C0488 32 21 3.905 5.00E-09 5.00E-09 C0488 32 22 4.261 5.80E-08 1.40E-08 C0488 32 23 4.611 9.90E-08 6.93E-09 C0488 32 24 5.008 2.90E-07 2.03E-08 C0488 32 25 5.125 4.10E-07 2.87E-08 C0488 32 26 5.388 7.20E-07 5.04E-08 C0488 32 27 5.643 1.10E-06 1.00E-07 C0488 32 28 6.038 3.30E-06 4.00E-07 C0488 32 29 6.316 3.60E-06 2.52E-07 C0488 32 30 ENDDATA 11 0 C0488 32 31 ENDSUBENT 30 0 C0488 3299999 SUBENT C0488033 20160321 C158C0488 33 1 BIB 3 10 C0488 33 2 REACTION (60-ND-143(P,N)61-PM-143,,PY,,TT) C0488 33 3 ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C0488 33 4 . either statistical, due to number of gamma counts, C0488 33 5 . or set to 7% due to uncertainties in of about 5% in C0488 33 6 bombardment parameters such as current integration C0488 33 7 and 5 % in counting due to source location, etc., C0488 33 8 added in quadrature. C0488 33 9 (ERR-1) Bombardment parameters. C0488 33 10 (ERR-2) Source location. C0488 33 11 STATUS (TABLE) Table II, page 188. C0488 33 12 ENDBIB 10 0 C0488 33 13 COMMON 2 3 C0488 33 14 ERR-1 ERR-2 C0488 33 15 PER-CENT PER-CENT C0488 33 16 5.0 5.0 C0488 33 17 ENDCOMMON 3 0 C0488 33 18 DATA 3 6 C0488 33 19 EN-CM DATA DATA-ERR C0488 33 20 MEV PRD/INC PRD/INC C0488 33 21 4.690 6.41E-08 2.14E-08 C0488 33 22 4.966 2.49E-07 7.11E-08 C0488 33 23 5.127 2.83E-07 8.90E-08 C0488 33 24 5.238 4.72E-07 8.90E-08 C0488 33 25 5.556 1.39E-06 2.09E-07 C0488 33 26 5.974 2.01E-06 3.02E-07 C0488 33 27 ENDDATA 8 0 C0488 33 28 ENDSUBENT 27 0 C0488 3399999 SUBENT C0488034 20160321 C158C0488 34 1 BIB 3 10 C0488 34 2 REACTION (60-ND-144(P,N)61-PM-144,,PY,,TT) C0488 34 3 ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C0488 34 4 . either statistical, due to number of gamma counts, C0488 34 5 . or set to 7% due to uncertainties in of about 5% in C0488 34 6 bombardment parameters such as current integration C0488 34 7 and 5 % in counting due to source location, etc., C0488 34 8 added in quadrature. C0488 34 9 (ERR-1) Bombardment parameters. C0488 34 10 (ERR-2) Source location. C0488 34 11 STATUS (TABLE) Table II, page 188. C0488 34 12 ENDBIB 10 0 C0488 34 13 COMMON 2 3 C0488 34 14 ERR-1 ERR-2 C0488 34 15 PER-CENT PER-CENT C0488 34 16 5.0 5.0 C0488 34 17 ENDCOMMON 3 0 C0488 34 18 DATA 3 7 C0488 34 19 EN-CM DATA DATA-ERR C0488 34 20 MEV PRD/INC PRD/INC C0488 34 21 3.850 6.20E-09 3.30E-09 C0488 34 22 4.690 5.23E-08 7.85E-09 C0488 34 23 4.967 9.20E-08 1.67E-08 C0488 34 24 5.128 1.51E-07 3.30E-08 C0488 34 25 5.238 2.05E-07 3.07E-08 C0488 34 26 5.556 6.32E-07 9.48E-08 C0488 34 27 5.974 1.46E-06 2.19E-07 C0488 34 28 ENDDATA 9 0 C0488 34 29 ENDSUBENT 28 0 C0488 3499999 SUBENT C0488035 20160321 C158C0488 35 1 BIB 3 10 C0488 35 2 REACTION (60-ND-146(P,N)61-PM-146,,PY,,TT) C0488 35 3 ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C0488 35 4 . either statistical, due to number of gamma counts, C0488 35 5 . or set to 7% due to uncertainties in of about 5% in C0488 35 6 bombardment parameters such as current integration C0488 35 7 and 5 % in counting due to source location, etc., C0488 35 8 added in quadrature. C0488 35 9 (ERR-1) Bombardment parameters. C0488 35 10 (ERR-2) Source location. C0488 35 11 STATUS (TABLE) Table II, page 188. C0488 35 12 ENDBIB 10 0 C0488 35 13 COMMON 2 3 C0488 35 14 ERR-1 ERR-2 C0488 35 15 PER-CENT PER-CENT C0488 35 16 5.0 5.0 C0488 35 17 ENDCOMMON 3 0 C0488 35 18 DATA 3 7 C0488 35 19 EN-CM DATA DATA-ERR C0488 35 20 MEV PRD/INC PRD/INC C0488 35 21 3.853 1.05E-08 9.00E-07 C0488 35 22 4.692 2.29E-07 1.58E-07 C0488 35 23 4.967 7.04E-07 6.04E-07 C0488 35 24 5.128 9.69E-07 3.52E-07 C0488 35 25 5.239 5.02E-07 3.51E-08 C0488 35 26 5.557 9.87E-07 2.64E-07 C0488 35 27 5.974 2.59E-06 3.89E-07 C0488 35 28 ENDDATA 9 0 C0488 35 29 ENDSUBENT 28 0 C0488 3599999 SUBENT C0488036 20160321 C158C0488 36 1 BIB 3 10 C0488 36 2 REACTION (60-ND-148(P,N)61-PM-148,,PY,,TT) C0488 36 3 ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C0488 36 4 . either statistical, due to number of gamma counts, C0488 36 5 . or set to 7% due to uncertainties in of about 5% in C0488 36 6 bombardment parameters such as current integration C0488 36 7 and 5 % in counting due to source location, etc., C0488 36 8 added in quadrature. C0488 36 9 (ERR-1) Bombardment parameters. C0488 36 10 (ERR-2) Source location. C0488 36 11 STATUS (TABLE) Table II, page 188. C0488 36 12 ENDBIB 10 0 C0488 36 13 COMMON 2 3 C0488 36 14 ERR-1 ERR-2 C0488 36 15 PER-CENT PER-CENT C0488 36 16 5.0 5.0 C0488 36 17 ENDCOMMON 3 0 C0488 36 18 DATA 3 9 C0488 36 19 EN-CM DATA DATA-ERR C0488 36 20 MEV PRD/INC PRD/INC C0488 36 21 3.854 5.70E-09 3.10E-09 C0488 36 22 4.310 7.30E-09 1.09E-09 C0488 36 23 4.559 3.14E-08 7.30E-09 C0488 36 24 4.692 5.22E-08 2.61E-08 C0488 36 25 4.967 7.33E-08 1.57E-08 C0488 36 26 5.128 1.25E-07 1.87E-08 C0488 36 27 5.239 2.03E-07 4.17E-08 C0488 36 28 5.557 3.66E-07 5.49E-08 C0488 36 29 5.975 7.89E-07 1.18E-07 C0488 36 30 ENDDATA 11 0 C0488 36 31 ENDSUBENT 30 0 C0488 3699999 SUBENT C0488037 20160321 C158C0488 37 1 BIB 3 10 C0488 37 2 REACTION (60-ND-148(P,N)61-PM-148-M,,PY,,TT) C0488 37 3 ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C0488 37 4 . either statistical, due to number of gamma counts, C0488 37 5 . or set to 7% due to uncertainties in of about 5% in C0488 37 6 bombardment parameters such as current integration C0488 37 7 and 5 % in counting due to source location, etc., C0488 37 8 added in quadrature. C0488 37 9 (ERR-1) Bombardment parameters. C0488 37 10 (ERR-2) Source location. C0488 37 11 STATUS (TABLE) Table II, page 188. C0488 37 12 ENDBIB 10 0 C0488 37 13 COMMON 2 3 C0488 37 14 ERR-1 ERR-2 C0488 37 15 PER-CENT PER-CENT C0488 37 16 5.0 5.0 C0488 37 17 ENDCOMMON 3 0 C0488 37 18 DATA 3 4 C0488 37 19 EN-CM DATA DATA-ERR C0488 37 20 MEV PRD/INC PRD/INC C0488 37 21 4.690 7.62E-08 3.20E-08 C0488 37 22 5.128 3.94E-07 5.91E-08 C0488 37 23 5.557 4.77E-07 7.16E-08 C0488 37 24 5.975 2.10E-06 3.15E-07 C0488 37 25 ENDDATA 6 0 C0488 37 26 ENDSUBENT 25 0 C0488 3799999 SUBENT C0488038 20160321 C158C0488 38 1 BIB 3 10 C0488 38 2 REACTION (60-ND-150(P,N)61-PM-150,,PY,,TT) C0488 38 3 ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C0488 38 4 . either statistical, due to number of gamma counts, C0488 38 5 . or set to 7% due to uncertainties in of about 5% in C0488 38 6 bombardment parameters such as current integration C0488 38 7 and 5 % in counting due to source location, etc., C0488 38 8 added in quadrature. C0488 38 9 (ERR-1) Bombardment parameters. C0488 38 10 (ERR-2) Source location. C0488 38 11 STATUS (TABLE) Table II, page 188. C0488 38 12 ENDBIB 10 0 C0488 38 13 COMMON 2 3 C0488 38 14 ERR-1 ERR-2 C0488 38 15 PER-CENT PER-CENT C0488 38 16 5.0 5.0 C0488 38 17 ENDCOMMON 3 0 C0488 38 18 DATA 3 12 C0488 38 19 EN-CM DATA DATA-ERR C0488 38 20 MEV PRD/INC PRD/INC C0488 38 21 2.994 9.70E-09 8.70E-09 C0488 38 22 3.494 6.76E-08 1.94E-08 C0488 38 23 3.546 1.85E-08 3.60E-09 C0488 38 24 3.854 7.73E-07 1.57E-07 C0488 38 25 3.988 8.68E-07 1.94E-07 C0488 38 26 4.311 3.38E-06 7.25E-07 C0488 38 27 4.559 4.47E-06 6.71E-07 C0488 38 28 4.693 5.81E-06 1.45E-06 C0488 38 29 4.968 9.18E-06 1.38E-06 C0488 38 30 5.129 1.91E-05 2.87E-06 C0488 38 31 5.240 1.90E-05 2.85E-06 C0488 38 32 5.976 1.76E-04 2.64E-05 C0488 38 33 ENDDATA 14 0 C0488 38 34 ENDSUBENT 33 0 C0488 3899999 SUBENT C0488039 20160321 C158C0488 39 1 BIB 3 10 C0488 39 2 REACTION (62-SM-147(P,N)63-EU-147,,PY,,TT) C0488 39 3 ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C0488 39 4 . either statistical, due to number of gamma counts, C0488 39 5 . or set to 7% due to uncertainties in of about 5% in C0488 39 6 bombardment parameters such as current integration C0488 39 7 and 5 % in counting due to source location, etc., C0488 39 8 added in quadrature. C0488 39 9 (ERR-1) Bombardment parameters. C0488 39 10 (ERR-2) Source location. C0488 39 11 STATUS (TABLE) Table II, page 188. C0488 39 12 ENDBIB 10 0 C0488 39 13 COMMON 2 3 C0488 39 14 ERR-1 ERR-2 C0488 39 15 PER-CENT PER-CENT C0488 39 16 5.0 5.0 C0488 39 17 ENDCOMMON 3 0 C0488 39 18 DATA 3 11 C0488 39 19 EN-CM DATA DATA-ERR C0488 39 20 MEV PRD/INC PRD/INC C0488 39 21 3.051 2.15E-09 2.15E-09 C0488 39 22 3.320 1.77E-10 1.80e-10 C0488 39 23 3.909 8.65E-09 3.60E-09 C0488 39 24 4.261 2.38E-08 9.00E-09 C0488 39 25 4.618 5.60E-08 6.50E-09 C0488 39 26 5.009 2.12E-07 5.00E-08 C0488 39 27 5.200 3.10E-07 3.60E-08 C0488 39 28 5.388 5.96E-07 5.40E-08 C0488 39 29 5.643 4.70E-07 2.20E-07 C0488 39 30 6.321 2.86E-06 7.20E-07 C0488 39 31 6.800 2.50E-06 9.00E-07 C0488 39 32 ENDDATA 13 0 C0488 39 33 ENDSUBENT 32 0 C0488 3999999 SUBENT C0488040 20160321 C158C0488 40 1 BIB 3 10 C0488 40 2 REACTION (62-SM-148(P,N)63-EU-148,,PY,,TT) C0488 40 3 ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C0488 40 4 . either statistical, due to number of gamma counts, C0488 40 5 . or set to 7% due to uncertainties in of about 5% in C0488 40 6 bombardment parameters such as current integration C0488 40 7 and 5 % in counting due to source location, etc., C0488 40 8 added in quadrature. C0488 40 9 (ERR-1) Bombardment parameters. C0488 40 10 (ERR-2) Source location. C0488 40 11 STATUS (TABLE) Table II, page 189. C0488 40 12 ENDBIB 10 0 C0488 40 13 COMMON 2 3 C0488 40 14 ERR-1 ERR-2 C0488 40 15 PER-CENT PER-CENT C0488 40 16 5.0 5.0 C0488 40 17 ENDCOMMON 3 0 C0488 40 18 DATA 3 9 C0488 40 19 EN-CM DATA DATA-ERR C0488 40 20 MEV PRD/INC PRD/INC C0488 40 21 3.905 1.80E-09 1.80E-09 C0488 40 22 4.260 3.60E-09 4.50E-09 C0488 40 23 4.610 2.66E-08 3.10E-09 C0488 40 24 5.009 1.46E-07 7.20E-08 C0488 40 25 5.199 1.67E-07 1.90E-08 C0488 40 26 5.390 1.93E-07 2.30E-08 C0488 40 27 5.650 3.70E-07 8.00E-08 C0488 40 28 6.312 2.25E-06 1.80E-07 C0488 40 29 6.799 4.32E-06 6.30E-07 C0488 40 30 ENDDATA 11 0 C0488 40 31 ENDSUBENT 30 0 C0488 4099999 SUBENT C0488041 20160321 C158C0488 41 1 BIB 3 10 C0488 41 2 REACTION (62-SM-149(P,N)63-EU-149,,PY,,TT) C0488 41 3 ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C0488 41 4 . either statistical, due to number of gamma counts, C0488 41 5 . or set to 7% due to uncertainties in of about 5% in C0488 41 6 bombardment parameters such as current integration C0488 41 7 and 5 % in counting due to source location, etc., C0488 41 8 added in quadrature. C0488 41 9 (ERR-1) Bombardment parameters. C0488 41 10 (ERR-2) Source location. C0488 41 11 STATUS (TABLE) Table II, page 189. C0488 41 12 ENDBIB 10 0 C0488 41 13 COMMON 2 3 C0488 41 14 ERR-1 ERR-2 C0488 41 15 PER-CENT PER-CENT C0488 41 16 5.0 5.0 C0488 41 17 ENDCOMMON 3 0 C0488 41 18 DATA 3 11 C0488 41 19 EN-CM DATA DATA-ERR C0488 41 20 MEV PRD/INC PRD/INC C0488 41 21 3.055 1.40E-08 1.40E-08 C0488 41 22 3.324 1.40E-08 4.50E-09 C0488 41 23 3.378 2.70E-08 9.00E-09 C0488 41 24 3.908 2.60E-08 1.70E-08 C0488 41 25 4.263 4.20E-08 1.10E-08 C0488 41 26 4.614 6.70E-08 1.70E-08 C0488 41 27 5.015 1.60E-07 8.00E-08 C0488 41 28 5.203 1.06E-07 6.00E-08 C0488 41 29 5.392 1.12E-07 6.00E-08 C0488 41 30 5.649 7.20E-07 5.00E-07 C0488 41 31 6.799 1.44E-06 4.40E-07 C0488 41 32 ENDDATA 13 0 C0488 41 33 ENDSUBENT 32 0 C0488 4199999 SUBENT C0488042 20160321 C158C0488 42 1 BIB 3 10 C0488 42 2 REACTION (62-SM-150(P,N)63-EU-150,,PY,,TT) C0488 42 3 ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C0488 42 4 . either statistical, due to number of gamma counts, C0488 42 5 . or set to 7% due to uncertainties in of about 5% in C0488 42 6 bombardment parameters such as current integration C0488 42 7 and 5 % in counting due to source location, etc., C0488 42 8 added in quadrature. C0488 42 9 (ERR-1) Bombardment parameters. C0488 42 10 (ERR-2) Source location. C0488 42 11 STATUS (TABLE) Table II, page 189. C0488 42 12 ENDBIB 10 0 C0488 42 13 COMMON 2 3 C0488 42 14 ERR-1 ERR-2 C0488 42 15 PER-CENT PER-CENT C0488 42 16 5.0 5.0 C0488 42 17 ENDCOMMON 3 0 C0488 42 18 DATA 3 9 C0488 42 19 EN-CM DATA DATA-ERR C0488 42 20 MEV PRD/INC PRD/INC C0488 42 21 3.378 3.20E-10 3.20E-10 C0488 42 22 4.264 1.00E-08 5.00E-09 C0488 42 23 4.614 4.20E-08 2.10E-08 C0488 42 24 5.016 8.00E-08 1.60E-08 C0488 42 25 5.203 1.10E-07 2.60E-08 C0488 42 26 5.392 1.50E-07 5.00E-08 C0488 42 27 5.649 3.10E-07 2.17E-08 C0488 42 28 6.318 1.33E-06 2.10E-07 C0488 42 29 6.797 3.10E-06 9.60E-07 C0488 42 30 ENDDATA 11 0 C0488 42 31 ENDSUBENT 30 0 C0488 4299999 SUBENT C0488043 20160321 C158C0488 43 1 BIB 3 10 C0488 43 2 REACTION (62-SM-152(P,N)63-EU-152,,PY,,TT) C0488 43 3 ERR-ANALYS (DATA-ERR) Uncertainty is the larger of C0488 43 4 . either statistical, due to number of gamma counts, C0488 43 5 . or set to 7% due to uncertainties in of about 5% in C0488 43 6 bombardment parameters such as current integration C0488 43 7 and 5 % in counting due to source location, etc., C0488 43 8 added in quadrature. C0488 43 9 (ERR-1) Bombardment parameters. C0488 43 10 (ERR-2) Source location. C0488 43 11 STATUS (TABLE) Table II, page 189. C0488 43 12 ENDBIB 10 0 C0488 43 13 COMMON 2 3 C0488 43 14 ERR-1 ERR-2 C0488 43 15 PER-CENT PER-CENT C0488 43 16 5.0 5.0 C0488 43 17 ENDCOMMON 3 0 C0488 43 18 DATA 3 11 C0488 43 19 EN-CM DATA DATA-ERR C0488 43 20 MEV PRD/INC PRD/INC C0488 43 21 3.054 2.70E-10 1.80E-10 C0488 43 22 3.379 5.72E-10 1.95E-10 C0488 43 23 3.908 3.77E-09 7.00E-10 C0488 43 24 4.264 1.10E-08 7.70E-10 C0488 43 25 4.615 3.19E-08 2.23E-09 C0488 43 26 5.016 1.09E-07 7.63E-09 C0488 43 27 5.204 1.56E-07 1.09E-08 C0488 43 28 5.393 1.70E-07 1.40E-08 C0488 43 29 5.650 4.76E-07 3.33E-08 C0488 43 30 6.318 1.88E-06 1.32E-07 C0488 43 31 6.800 3.37E-06 2.36E-07 C0488 43 32 ENDDATA 13 0 C0488 43 33 ENDSUBENT 32 0 C0488 4399999 SUBENT C0488044 20160323 C158C0488 44 1 BIB 5 13 C0488 44 2 REACTION (5-B-10(P,A)4-BE-7,,SGV) C0488 44 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488 44 4 directly from measured reaction cross sections and C0488 44 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488 44 7 value of the product of the cross section times the C0488 44 8 velocity, averaged over the Maxwell-Boltzmann C0488 44 9 velocity distribution at the temperature T of interest.C0488 44 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488 44 11 their values were added quadratically. C0488 44 12 STATUS (TABLE) Table III, page 190. C0488 44 13 (DEP,C0487002) C0488 44 14 HISTORY (20160323C) BP C0488 44 15 ENDBIB 13 0 C0488 44 16 NOCOMMON 0 0 C0488 44 17 DATA 3 14 C0488 44 18 KT DATA DATA-ERR C0488 44 19 K9 CM3/S/MOL CM3/S/MOL C0488 44 20 .500 1.90E+5 2.85E+4 C0488 44 21 1.000 1.44E+6 2.16E+5 C0488 44 22 1.500 4.64E+6 6.96E+5 C0488 44 23 2.000 1.10E+7 1.65E+6 C0488 44 24 2.500 2.08E+7 3.12E+6 C0488 44 25 3.000 3.30E+7 4.95E+6 C0488 44 26 3.500 4.64E+7 6.96E+6 C0488 44 27 4.000 6.01E+7 9.02E+6 C0488 44 28 4.500 7.32E+7 1.10E+6 C0488 44 29 5.000 8.52E+7 1.28E+7 C0488 44 30 5.500 9.60E+7 1.44E+7 C0488 44 31 6.000 1.05E+8 1.58E+7 C0488 44 32 6.500 1.13E+8 2.70E+7 C0488 44 33 7.000 1.20E+8 2.10E+7 C0488 44 34 ENDDATA 16 0 C0488 44 35 ENDSUBENT 34 0 C0488 4499999 SUBENT C0488045 20160323 C158C0488 45 1 BIB 5 13 C0488 45 2 REACTION (5-B-10(P,G)6-C-11,,SGV,,MXW) C0488 45 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488 45 4 directly from measured reaction cross sections and C0488 45 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488 45 7 value of the product of the cross section times the C0488 45 8 velocity, averaged over the Maxwell-Boltzmann C0488 45 9 velocity distribution at the temperature T of interest.C0488 45 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488 45 11 their values were added quadratically. C0488 45 12 STATUS (TABLE) Table III, page 190. C0488 45 13 (DEP,C0487003) C0488 45 14 HISTORY (20160323C) BP C0488 45 15 ENDBIB 13 0 C0488 45 16 NOCOMMON 0 0 C0488 45 17 DATA 3 11 C0488 45 18 KT DATA DATA-ERR C0488 45 19 K9 CM3/S/MOL CM3/S/MOL C0488 45 20 2.000 3.93E+2 5.90E+1 C0488 45 21 2.500 6.50E+2 9.87E+1 C0488 45 22 3.000 9.62E+2 1.44E+2 C0488 45 23 3.500 1.28E+3 1.92E+2 C0488 45 24 4.000 1.60E+3 2.40E+2 C0488 45 25 4.500 1.91E+3 2.87E+2 C0488 45 26 5.000 2.21E+3 3.32E+2 C0488 45 27 5.500 2.40E+3 3.89E+2 C0488 45 28 6.000 2.72E+3 5.52E+2 C0488 45 29 6.500 2.93E+3 7.42E+2 C0488 45 30 7.000 3.12E+3 9.57E+2 C0488 45 31 ENDDATA 13 0 C0488 45 32 ENDSUBENT 31 0 C0488 4599999 SUBENT C0488046 20160323 C158C0488 46 1 BIB 5 13 C0488 46 2 REACTION (6-C-12(P,G)7-N-13,,SGV) C0488 46 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488 46 4 directly from measured reaction cross sections and C0488 46 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488 46 7 value of the product of the cross section times the C0488 46 8 velocity, averaged over the Maxwell-Boltzmann C0488 46 9 velocity distribution at the temperature T of interest.C0488 46 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488 46 11 their values were added quadratically. C0488 46 12 STATUS (TABLE) Table III, page 190. C0488 46 13 (DEP,C0487004) C0488 46 14 HISTORY (20160323C) BP C0488 46 15 ENDBIB 13 0 C0488 46 16 NOCOMMON 0 0 C0488 46 17 DATA 3 13 C0488 46 18 KT DATA DATA-ERR C0488 46 19 K9 CM3/S/MOL CM3/S/MOL C0488 46 20 1.000 7.27E+2 1.09E+2 C0488 46 21 1.500 1.96E+3 2.94E+2 C0488 46 22 2.000 2.90E+3 4.35E+2 C0488 46 23 2.500 3.44E+3 5.16E+2 C0488 46 24 3.000 3.72E+3 5.58E+2 C0488 46 25 3.500 3.85E+3 5.76E+2 C0488 46 26 4.000 3.89E+3 5.84E+2 C0488 46 27 4.500 3.89E+3 5.84E+2 C0488 46 28 5.000 3.85E+3 5.78E+2 C0488 46 29 5.500 3.80E+3 5.70E+2 C0488 46 30 6.000 3.74E+3 5.61E+2 C0488 46 31 6.500 3.66E+3 5.49E+2 C0488 46 32 7.000 3.59E+3 6.61E+2 C0488 46 33 ENDDATA 15 0 C0488 46 34 ENDSUBENT 33 0 C0488 4699999 SUBENT C0488047 20160323 C158C0488 47 1 BIB 5 13 C0488 47 2 REACTION (7-N-14(P,G)8-O-15,,SGV) C0488 47 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488 47 4 directly from measured reaction cross sections and C0488 47 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488 47 7 value of the product of the cross section times the C0488 47 8 velocity, averaged over the Maxwell-Boltzmann C0488 47 9 velocity distribution at the temperature T of interest.C0488 47 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488 47 11 their values were added quadratically. C0488 47 12 STATUS (TABLE) Table III, page 190. C0488 47 13 (DEP,C0488002) C0488 47 14 HISTORY (20160323C) BP C0488 47 15 ENDBIB 13 0 C0488 47 16 NOCOMMON 0 0 C0488 47 17 DATA 3 11 C0488 47 18 KT DATA DATA-ERR C0488 47 19 K9 CM3/S/MOL CM3/S/MOL C0488 47 20 1.500 4.96E+2 2.54E+2 C0488 47 21 2.000 6.85E+2 1.68E+2 C0488 47 22 2.500 9.84E+2 1.48E+2 C0488 47 23 3.000 1.41E+3 2.12E+2 C0488 47 24 3.500 1.91E+3 2.96E+2 C0488 47 25 4.000 2.64E+3 3.96E+2 C0488 47 26 4.500 3.40E+3 5.96E+2 C0488 47 27 5.000 4.22E+3 1.03E+3 C0488 47 28 5.500 5.06E+3 1.63E+3 C0488 47 29 6.000 5.90E+3 2.40E+3 C0488 47 30 6.500 6.72E+3 3.33E+3 C0488 47 31 ENDDATA 13 0 C0488 47 32 ENDSUBENT 31 0 C0488 4799999 SUBENT C0488048 20160323 C158C0488 48 1 BIB 5 13 C0488 48 2 REACTION (14-SI-28(P,G)15-P-29,,SGV) C0488 48 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488 48 4 directly from measured reaction cross sections and C0488 48 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488 48 7 value of the product of the cross section times the C0488 48 8 velocity, averaged over the Maxwell-Boltzmann C0488 48 9 velocity distribution at the temperature T of interest.C0488 48 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488 48 11 their values were added quadratically. C0488 48 12 STATUS (TABLE) Table III, page 190. C0488 48 13 (DEP,C0487005) C0488 48 14 HISTORY (20160323C) BP C0488 48 15 ENDBIB 13 0 C0488 48 16 NOCOMMON 0 0 C0488 48 17 DATA 3 12 C0488 48 18 KT DATA DATA-ERR C0488 48 19 K9 CM3/S/MOL CM3/S/MOL C0488 48 20 1.500 2.64E+0 5.52E-1 C0488 48 21 2.000 2.87E+1 4.31E+0 C0488 48 22 2.500 1.21E+2 1.81E+1 C0488 48 23 3.000 3.10E+2 4.65E+1 C0488 48 24 3.500 5.97E+2 8.96E+1 C0488 48 25 4.000 9.64E+2 1.45E+2 C0488 48 26 4.500 1.38E+3 2.07E+2 C0488 48 27 5.000 1.83E+3 2.75E+2 C0488 48 28 5.500 2.28E+3 3.42E+2 C0488 48 29 6.000 2.71E+3 4.07E+2 C0488 48 30 6.500 3.13E+3 4.70E+2 C0488 48 31 7.000 3.51E+3 5.98E+2 C0488 48 32 ENDDATA 14 0 C0488 48 33 ENDSUBENT 32 0 C0488 4899999 SUBENT C0488049 20160323 C158C0488 49 1 BIB 5 13 C0488 49 2 REACTION (14-SI-29(P,G)15-P-30,,SGV) C0488 49 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488 49 4 directly from measured reaction cross sections and C0488 49 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488 49 7 value of the product of the cross section times the C0488 49 8 velocity, averaged over the Maxwell-Boltzmann C0488 49 9 velocity distribution at the temperature T of interest.C0488 49 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488 49 11 their values were added quadratically. C0488 49 12 STATUS (TABLE) Table III, page 190. C0488 49 13 (DEP,C0487006) C0488 49 14 HISTORY (20160323C) BP C0488 49 15 ENDBIB 13 0 C0488 49 16 NOCOMMON 0 0 C0488 49 17 DATA 3 10 C0488 49 18 KT DATA DATA-ERR C0488 49 19 K9 CM3/S/MOL CM3/S/MOL C0488 49 20 2.000 2.84E+3 7.78E+2 C0488 49 21 2.500 3.55E+3 5.47E+2 C0488 49 22 3.000 4.40E+3 6.60E+2 C0488 49 23 3.500 5.48E+3 8.22E+2 C0488 49 24 4.000 6.81E+3 1.02E+3 C0488 49 25 4.500 8.35E+3 1.25E+3 C0488 49 26 5.000 1.01E+4 1.52E+3 C0488 49 27 5.500 1.19E+4 1.79E+3 C0488 49 28 6.000 1.37E+4 2.06E+3 C0488 49 29 6.500 1.55E+4 2.33E+3 C0488 49 30 ENDDATA 12 0 C0488 49 31 ENDSUBENT 30 0 C0488 4999999 SUBENT C0488050 20160323 C158C0488 50 1 BIB 5 13 C0488 50 2 REACTION (20-CA-40(P,G)21-SC-41,,SGV) C0488 50 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488 50 4 directly from measured reaction cross sections and C0488 50 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488 50 7 value of the product of the cross section times the C0488 50 8 velocity, averaged over the Maxwell-Boltzmann C0488 50 9 velocity distribution at the temperature T of interest.C0488 50 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488 50 11 their values were added quadratically. C0488 50 12 STATUS (TABLE) Table III, page 190. C0488 50 13 (DEP,C0487007) C0488 50 14 HISTORY (20160323C) BP C0488 50 15 ENDBIB 13 0 C0488 50 16 NOCOMMON 0 0 C0488 50 17 DATA 3 10 C0488 50 18 KT DATA DATA-ERR C0488 50 19 K9 CM3/S/MOL CM3/S/MOL C0488 50 20 3.500 3.25E+1 9.62E+0 C0488 50 21 4.000 4.51E+1 8.77E+0 C0488 50 22 4.500 6.17E+1 9.25E+0 C0488 50 23 5.000 8.28E+1 1.24E+1 C0488 50 24 5.500 1.09E+2 1.64E+1 C0488 50 25 6.000 1.40E+2 2.10E+1 C0488 50 26 6.500 1.77E+2 2.66E+1 C0488 50 27 7.000 2.17E+2 3.25E+1 C0488 50 28 7.500 2.62E+2 3.93E+1 C0488 50 29 8.000 3.11E+2 5.55E+1 C0488 50 30 ENDDATA 12 0 C0488 50 31 ENDSUBENT 30 0 C0488 5099999 SUBENT C0488051 20160323 C158C0488 51 1 BIB 5 13 C0488 51 2 REACTION (22-TI-46(P,G)23-V-47,,SGV) C0488 51 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488 51 4 directly from measured reaction cross sections and C0488 51 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488 51 7 value of the product of the cross section times the C0488 51 8 velocity, averaged over the Maxwell-Boltzmann C0488 51 9 velocity distribution at the temperature T of interest.C0488 51 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488 51 11 their values were added quadratically. C0488 51 12 STATUS (TABLE) Table III, page 190. C0488 51 13 (DEP,C0487008) C0488 51 14 HISTORY (20160323C) BP C0488 51 15 ENDBIB 13 0 C0488 51 16 NOCOMMON 0 0 C0488 51 17 DATA 3 12 C0488 51 18 KT DATA DATA-ERR C0488 51 19 K9 CM3/S/MOL CM3/S/MOL C0488 51 20 1.500 2.16E+2 3.24E+1 C0488 51 21 2.000 9.49E+2 1.42E+2 C0488 51 22 2.500 2.50E+3 3.75E+2 C0488 51 23 3.000 4.98E+3 7.47E+2 C0488 51 24 3.500 8.35E+3 1.25E+3 C0488 51 25 4.000 1.25E+4 1.88E+3 C0488 51 26 4.500 1.72E+4 2.58E+3 C0488 51 27 5.000 2.23E+4 3.35E+3 C0488 51 28 5.500 2.77E+4 4.16E+3 C0488 51 29 6.000 3.31E+4 4.97E+3 C0488 51 30 6.500 3.85E+4 5.97E+3 C0488 51 31 7.000 4.37E+4 8.48E+3 C0488 51 32 ENDDATA 14 0 C0488 51 33 ENDSUBENT 32 0 C0488 5199999 SUBENT C0488052 20160323 C158C0488 52 1 BIB 5 13 C0488 52 2 REACTION (22-TI-47(P,G)23-V-48,,SGV) C0488 52 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488 52 4 directly from measured reaction cross sections and C0488 52 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488 52 7 value of the product of the cross section times the C0488 52 8 velocity, averaged over the Maxwell-Boltzmann C0488 52 9 velocity distribution at the temperature T of interest.C0488 52 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488 52 11 their values were added quadratically. C0488 52 12 STATUS (TABLE) Table III, page 190. C0488 52 13 (DEP,C0487009) C0488 52 14 HISTORY (20160323C) BP C0488 52 15 ENDBIB 13 0 C0488 52 16 NOCOMMON 0 0 C0488 52 17 DATA 3 12 C0488 52 18 KT DATA DATA-ERR C0488 52 19 K9 CM3/S/MOL CM3/S/MOL C0488 52 20 1.500 3.47E+2 6.18E+1 C0488 52 21 2.000 1.83E+3 2.75E+2 C0488 52 22 2.500 5.42E+3 8.13E+2 C0488 52 23 3.000 1.17E+4 1.76E+3 C0488 52 24 3.500 2.09E+4 3.14E+3 C0488 52 25 4.000 3.29E+4 4.94E+3 C0488 52 26 4.500 4.72E+4 7.08E+3 C0488 52 27 5.000 6.36E+4 9.54E+3 C0488 52 28 5.500 8.14E+4 1.22E+4 C0488 52 29 6.000 1.00E+5 1.50E+4 C0488 52 30 6.500 1.20E+5 1.80E+4 C0488 52 31 7.000 1.39E+5 2.09E+4 C0488 52 32 ENDDATA 14 0 C0488 52 33 ENDSUBENT 32 0 C0488 5299999 SUBENT C0488053 20160323 C158C0488 53 1 BIB 5 13 C0488 53 2 REACTION (24-CR-50(P,G)25-MN-51,,SGV) C0488 53 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488 53 4 directly from measured reaction cross sections and C0488 53 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488 53 7 value of the product of the cross section times the C0488 53 8 velocity, averaged over the Maxwell-Boltzmann C0488 53 9 velocity distribution at the temperature T of interest.C0488 53 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488 53 11 their values were added quadratically. C0488 53 12 STATUS (TABLE) Table III, page 190. C0488 53 13 (DEP,C0487010) C0488 53 14 HISTORY (20160323C) BP C0488 53 15 ENDBIB 13 0 C0488 53 16 NOCOMMON 0 0 C0488 53 17 DATA 3 13 C0488 53 18 KT DATA DATA-ERR C0488 53 19 K9 CM3/S/MOL CM3/S/MOL C0488 53 20 1.000 1.99E+0 4.22E-1 C0488 53 21 1.500 5.45E+1 8.18E+0 C0488 53 22 2.000 2.98E+2 4.47E+1 C0488 53 23 2.500 8.74E+2 1.31E+2 C0488 53 24 3.000 1.58E+3 2.82E+2 C0488 53 25 3.000 3.36E+3 5.04E+2 C0488 53 26 4.000 5.31E+3 7.97E+2 C0488 53 27 4.500 7.72E+3 1.16E+3 C0488 53 28 5.000 1.05E+4 1.58E+3 C0488 53 29 5.500 1.37E+4 2.06E+3 C0488 53 30 6.000 1.72E+4 2.58E+3 C0488 53 31 6.500 2.09E+4 3.14E+3 C0488 53 32 7.000 2.48E+4 3.72E+3 C0488 53 33 ENDDATA 15 0 C0488 53 34 ENDSUBENT 33 0 C0488 5399999 SUBENT C0488054 20160323 C158C0488 54 1 BIB 5 13 C0488 54 2 REACTION (26-FE-54(P,G)27-CO-55,,SGV) C0488 54 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488 54 4 directly from measured reaction cross sections and C0488 54 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488 54 7 value of the product of the cross section times the C0488 54 8 velocity, averaged over the Maxwell-Boltzmann C0488 54 9 velocity distribution at the temperature T of interest.C0488 54 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488 54 11 their values were added quadratically. C0488 54 12 STATUS (TABLE) Table III, page 190. C0488 54 13 (DEP,C0487011) C0488 54 14 HISTORY (20160323C) BP C0488 54 15 ENDBIB 13 0 C0488 54 16 NOCOMMON 0 0 C0488 54 17 DATA 3 10 C0488 54 18 KT DATA DATA-ERR C0488 54 19 K9 CM3/S/MOL CM3/S/MOL C0488 54 20 2.500 2.78E+2 7.28E+1 C0488 54 21 3.000 5.28E+2 7.92E+1 C0488 54 22 3.500 9.16E+2 1.37E+2 C0488 54 23 4.000 1.46E+3 2.19E+2 C0488 54 24 4.500 2.16E+3 3.24E+2 C0488 54 25 5.000 2.99E+3 4.49E+2 C0488 54 26 5.500 3.94E+3 5.91E+2 C0488 54 27 6.000 4.96E+3 8.44E+2 C0488 54 28 6.500 6.02E+3 1.27E+3 C0488 54 29 7.000 7.10E+3 1.81E+3 C0488 54 30 ENDDATA 12 0 C0488 54 31 ENDSUBENT 30 0 C0488 5499999 SUBENT C0488055 20160323 C158C0488 55 1 BIB 5 13 C0488 55 2 REACTION (26-FE-56(P,G)27-CO-57,,SGV) C0488 55 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488 55 4 directly from measured reaction cross sections and C0488 55 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488 55 7 value of the product of the cross section times the C0488 55 8 velocity, averaged over the Maxwell-Boltzmann C0488 55 9 velocity distribution at the temperature T of interest.C0488 55 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488 55 11 their values were added quadratically. C0488 55 12 STATUS (TABLE) Table III, page 190. C0488 55 13 (DEP,C0487012) C0488 55 14 HISTORY (20160323C) BP C0488 55 15 ENDBIB 13 0 C0488 55 16 NOCOMMON 0 0 C0488 55 17 DATA 3 5 C0488 55 18 KT DATA DATA-ERR C0488 55 19 K9 CM3/S/MOL CM3/S/MOL C0488 55 20 1.500 8.86E+1 4.98E+1 C0488 55 21 2.000 3.57E+2 1.11E+2 C0488 55 22 2.500 8.62E+2 2.85E+2 C0488 55 23 3.000 1.55E+3 6.98E+2 C0488 55 24 3.500 2.33E+3 1.39E+3 C0488 55 25 ENDDATA 7 0 C0488 55 26 ENDSUBENT 25 0 C0488 5599999 SUBENT C0488056 20160323 C158C0488 56 1 BIB 5 13 C0488 56 2 REACTION (28-NI-58(P,G)29-CU-59,,SGV) C0488 56 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488 56 4 directly from measured reaction cross sections and C0488 56 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488 56 7 value of the product of the cross section times the C0488 56 8 velocity, averaged over the Maxwell-Boltzmann C0488 56 9 velocity distribution at the temperature T of interest.C0488 56 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488 56 11 their values were added quadratically. C0488 56 12 STATUS (TABLE) Table III, page 190. C0488 56 13 (DEP,C0487013) C0488 56 14 HISTORY (20160323C) BP C0488 56 15 ENDBIB 13 0 C0488 56 16 NOCOMMON 0 0 C0488 56 17 DATA 3 8 C0488 56 18 KT DATA DATA-ERR C0488 56 19 K9 CM3/S/MOL CM3/S/MOL C0488 56 20 2.500 1.03E+2 3.00E+1 C0488 56 21 3.000 2.45E+2 4.62E+1 C0488 56 22 3.500 4.71E+2 7.07E+1 C0488 56 23 4.000 7.92E+2 1.19E+2 C0488 56 24 4.500 1.21E+3 1.82E+2 C0488 56 25 5.000 1.73E+3 3.05E+2 C0488 56 26 5.500 2.34E+3 5.67E+2 C0488 56 27 6.000 3.02E+3 4.53E+2 C0488 56 28 ENDDATA 10 0 C0488 56 29 ENDSUBENT 28 0 C0488 5699999 SUBENT C0488057 20160323 C158C0488 57 1 BIB 5 13 C0488 57 2 REACTION (28-NI-60(P,G)29-CU-61,,SGV) C0488 57 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488 57 4 directly from measured reaction cross sections and C0488 57 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488 57 7 value of the product of the cross section times the C0488 57 8 velocity, averaged over the Maxwell-Boltzmann C0488 57 9 velocity distribution at the temperature T of interest.C0488 57 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488 57 11 their values were added quadratically. C0488 57 12 STATUS (TABLE) Table III, page 190. C0488 57 13 (DEP,C0487014) C0488 57 14 HISTORY (20160323C) BP C0488 57 15 ENDBIB 13 0 C0488 57 16 NOCOMMON 0 0 C0488 57 17 DATA 3 12 C0488 57 18 KT DATA DATA-ERR C0488 57 19 K9 CM3/S/MOL CM3/S/MOL C0488 57 20 1.500 1.28E+1 1.92E+0 C0488 57 21 2.000 1.16E+2 1.74E+1 C0488 57 22 2.500 4.93E+2 7.40E+1 C0488 57 23 3.000 1.35E+3 2.03E+2 C0488 57 24 3.500 2.83E+3 4.25E+2 C0488 57 25 4.000 4.95E+3 7.43E+2 C0488 57 26 4.500 7.64E+3 1.15E+3 C0488 57 27 5.000 1.08E+4 2.02E+3 C0488 57 28 5.500 1.42E+4 3.42E+3 C0488 57 29 6.000 1.78E+4 5.32E+3 C0488 57 30 6.500 2.14E+4 7.70E+3 C0488 57 31 7.000 2.49E+4 1.05E+4 C0488 57 32 ENDDATA 14 0 C0488 57 33 ENDSUBENT 32 0 C0488 5799999 SUBENT C0488058 20160323 C158C0488 58 1 BIB 5 13 C0488 58 2 REACTION (28-NI-61(P,G)29-CU-62,,SGV) C0488 58 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488 58 4 directly from measured reaction cross sections and C0488 58 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488 58 7 value of the product of the cross section times the C0488 58 8 velocity, averaged over the Maxwell-Boltzmann C0488 58 9 velocity distribution at the temperature T of interest.C0488 58 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488 58 11 their values were added quadratically. C0488 58 12 STATUS (TABLE) Table III, page 190. C0488 58 13 (DEP,C0487015) C0488 58 14 HISTORY (20160323C) BP C0488 58 15 ENDBIB 13 0 C0488 58 16 NOCOMMON 0 0 C0488 58 17 DATA 3 12 C0488 58 18 KT DATA DATA-ERR C0488 58 19 K9 CM3/S/MOL CM3/S/MOL C0488 58 20 1.500 3.21E+1 4.81E+0 C0488 58 21 2.000 3.17E+2 4.76E+1 C0488 58 22 2.500 1.38E+3 2.07E+2 C0488 58 23 3.000 3.93E+3 5.90E+2 C0488 58 24 3.500 8.71E+3 1.31E+3 C0488 58 25 4.000 1.62E+4 2.43E+3 C0488 58 26 4.500 2.66E+4 3.99E+3 C0488 58 27 5.000 3.97E+4 5.96E+3 C0488 58 28 5.500 5.52E+4 9.33E+3 C0488 58 29 6.000 7.25E+4 1.57E+4 C0488 58 30 6.500 9.11E+4 2.44E+4 C0488 58 31 7.000 1.10E+5 3.53E+4 C0488 58 32 ENDDATA 14 0 C0488 58 33 ENDSUBENT 32 0 C0488 5899999 SUBENT C0488059 20160323 C158C0488 59 1 BIB 5 13 C0488 59 2 REACTION (30-ZN-64(P,G)31-GA-65,,SGV) C0488 59 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488 59 4 directly from measured reaction cross sections and C0488 59 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488 59 7 value of the product of the cross section times the C0488 59 8 velocity, averaged over the Maxwell-Boltzmann C0488 59 9 velocity distribution at the temperature T of interest.C0488 59 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488 59 11 their values were added quadratically. C0488 59 12 STATUS (TABLE) Table III, page 191. C0488 59 13 (DEP,C0487016) C0488 59 14 HISTORY (20160323C) BP C0488 59 15 ENDBIB 13 0 C0488 59 16 NOCOMMON 0 0 C0488 59 17 DATA 3 13 C0488 59 18 KT DATA DATA-ERR C0488 59 19 K9 CM3/S/MOL CM3/S/MOL C0488 59 20 1.000 8.11E-2 1.22E-2 C0488 59 21 1.500 5.31E+0 7.97E-1 C0488 59 22 2.000 6.00E+1 9.00E+0 C0488 59 23 2.500 2.97E+2 4.46E+1 C0488 59 24 3.000 9.31E+2 1.40E+2 C0488 59 25 3.500 2.20E+3 3.30E+2 C0488 59 26 4.000 4.32E+3 6.48E+2 C0488 59 27 4.500 7.44E+3 1.12E+3 C0488 59 28 5.000 1.16E+4 1.74E+3 C0488 59 29 5.500 1.69E+4 2.54E+3 C0488 59 30 6.000 2.33E+4 3.50E+3 C0488 59 31 6.500 3.05E+4 4.58E+3 C0488 59 32 7.000 3.86E+4 5.79E+3 C0488 59 33 ENDDATA 15 0 C0488 59 34 ENDSUBENT 33 0 C0488 5999999 SUBENT C0488060 20160323 C158C0488 60 1 BIB 5 13 C0488 60 2 REACTION (30-ZN-67(P,G)31-GA-68,,SGV) C0488 60 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488 60 4 directly from measured reaction cross sections and C0488 60 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488 60 7 value of the product of the cross section times the C0488 60 8 velocity, averaged over the Maxwell-Boltzmann C0488 60 9 velocity distribution at the temperature T of interest.C0488 60 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488 60 11 their values were added quadratically. C0488 60 12 STATUS (TABLE) Table III, page 191. C0488 60 13 (DEP,C0487017) C0488 60 14 HISTORY (20160323C) BP C0488 60 15 ENDBIB 13 0 C0488 60 16 NOCOMMON 0 0 C0488 60 17 DATA 3 13 C0488 60 18 KT DATA DATA-ERR C0488 60 19 K9 CM3/S/MOL CM3/S/MOL C0488 60 20 1.000 2.52E-1 3.78E-2 C0488 60 21 1.500 2.15E+1 3.23E+0 C0488 60 22 2.000 2.53E+2 3.80E+1 C0488 60 23 2.500 1.22E+3 1.83E+2 C0488 60 24 3.000 3.64E+3 5.46E+2 C0488 60 25 3.500 8.11E+3 1.22E+3 C0488 60 26 4.000 1.50E+4 2.25E+3 C0488 60 27 4.500 2.43E+4 3.65E+3 C0488 60 28 5.000 3.58E+4 5.37E+3 C0488 60 29 5.500 4.91E+4 7.37E+3 C0488 60 30 6.000 6.38E+4 9.57E+3 C0488 60 31 6.500 7.95E+4 1.41E+4 C0488 60 32 7.000 9.57E+4 2.08E+4 C0488 60 33 ENDDATA 15 0 C0488 60 34 ENDSUBENT 33 0 C0488 6099999 SUBENT C0488061 20160323 C158C0488 61 1 BIB 5 13 C0488 61 2 REACTION (32-GE-70(P,G)33-AS-71,,SGV) C0488 61 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488 61 4 directly from measured reaction cross sections and C0488 61 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488 61 7 value of the product of the cross section times the C0488 61 8 velocity, averaged over the Maxwell-Boltzmann C0488 61 9 velocity distribution at the temperature T of interest.C0488 61 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488 61 11 their values were added quadratically. C0488 61 12 STATUS (TABLE) Table III, page 191. C0488 61 13 (DEP,C0487018) C0488 61 14 HISTORY (20160323C) BP C0488 61 15 ENDBIB 13 0 C0488 61 16 NOCOMMON 0 0 C0488 61 17 DATA 3 11 C0488 61 18 KT DATA DATA-ERR C0488 61 19 K9 CM3/S/MOL CM3/S/MOL C0488 61 20 2.000 5.59E+1 1.60E+1 C0488 61 21 2.500 3.58E+2 5.37E+1 C0488 61 22 3.000 1.38E+3 2.07E+2 C0488 61 23 3.800 3.92E+3 5.88E+2 C0488 61 24 4.000 8.98E+3 1.35E+3 C0488 61 25 4.500 1.77E+4 2.66E+3 C0488 61 26 5.000 3.10E+4 4.65E+3 C0488 61 27 5.500 4.99E+4 7.49E+3 C0488 61 28 6.000 7.47E+4 1.12E+4 C0488 61 29 6.500 1.06E+5 1.59E+4 C0488 61 30 7.000 1.43E+5 2.35E+4 C0488 61 31 ENDDATA 13 0 C0488 61 32 ENDSUBENT 31 0 C0488 6199999 SUBENT C0488062 20160323 C158C0488 62 1 BIB 5 13 C0488 62 2 REACTION (38-SR-87(P,G)39-Y-88,,SGV) C0488 62 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488 62 4 directly from measured reaction cross sections and C0488 62 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488 62 7 value of the product of the cross section times the C0488 62 8 velocity, averaged over the Maxwell-Boltzmann C0488 62 9 velocity distribution at the temperature T of interest.C0488 62 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488 62 11 their values were added quadratically. C0488 62 12 STATUS (TABLE) Table III, page 191. C0488 62 13 (DEP,C0488003) C0488 62 14 HISTORY (20160323C) BP C0488 62 15 ENDBIB 13 0 C0488 62 16 NOCOMMON 0 0 C0488 62 17 DATA 3 9 C0488 62 18 KT DATA DATA-ERR C0488 62 19 K9 CM3/S/MOL CM3/S/MOL C0488 62 20 5.000 5.59E+5 1.78E+5 C0488 62 21 5.500 8.65E+5 2.02E+5 C0488 62 22 6.000 1.25E+6 2.36E+5 C0488 62 23 6.500 1.71E+6 2.94E+5 C0488 62 24 7.000 2.23E+6 3.87E+5 C0488 62 25 7.500 2.81E+6 5.37E+5 C0488 62 26 8.000 3.44E+6 7.61E+5 C0488 62 27 8.500 4.10E+6 1.13E+6 C0488 62 28 9.000 4.79E+6 1.51E+6 C0488 62 29 ENDDATA 11 0 C0488 62 30 ENDSUBENT 29 0 C0488 6299999 SUBENT C0488063 20160323 C158C0488 63 1 BIB 5 13 C0488 63 2 REACTION (40-ZR-90(P,G)41-NB-91-M,,SGV) C0488 63 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488 63 4 directly from measured reaction cross sections and C0488 63 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488 63 7 value of the product of the cross section times the C0488 63 8 velocity, averaged over the Maxwell-Boltzmann C0488 63 9 velocity distribution at the temperature T of interest.C0488 63 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488 63 11 their values were added quadratically. C0488 63 12 STATUS (TABLE) Table III, page 191. C0488 63 13 (DEP,C0488004) C0488 63 14 HISTORY (20160323C) BP C0488 63 15 ENDBIB 13 0 C0488 63 16 NOCOMMON 0 0 C0488 63 17 DATA 3 12 C0488 63 18 KT DATA DATA-ERR C0488 63 19 K9 CM3/S/MOL CM3/S/MOL C0488 63 20 2.500 7.27E+1 4.15E+1 C0488 63 21 3.000 2.76E+2 8.36E+1 C0488 63 22 3.500 8.15E+2 1.33E+2 C0488 63 23 4.000 2.04E+3 3.06E+2 C0488 63 24 4.500 4.53E+3 6.80E+2 C0488 63 25 5.000 9.08E+3 1.36E+3 C0488 63 26 5.500 1.61E+4 2.51E+3 C0488 63 27 6.000 2.86E+4 4.29E+3 C0488 63 28 6.500 4.60E+4 8.90E+3 C0488 63 29 7.000 7.00E+4 1.05E+4 C0488 63 30 7.500 1.01E+5 1.52E+4 C0488 63 31 8.000 1.41E+5 2.45E+4 C0488 63 32 ENDDATA 14 0 C0488 63 33 ENDSUBENT 32 0 C0488 6399999 SUBENT C0488064 20160323 C158C0488 64 1 BIB 5 13 C0488 64 2 REACTION (42-MO-92(P,G)43-TC-93,,SGV) C0488 64 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488 64 4 directly from measured reaction cross sections and C0488 64 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488 64 7 value of the product of the cross section times the C0488 64 8 velocity, averaged over the Maxwell-Boltzmann C0488 64 9 velocity distribution at the temperature T of interest.C0488 64 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488 64 11 their values were added quadratically. C0488 64 12 STATUS (TABLE) Table III, page 191. C0488 64 13 (DEP,C0487019) C0488 64 14 HISTORY (20160323C) BP C0488 64 15 ENDBIB 13 0 C0488 64 16 NOCOMMON 0 0 C0488 64 17 DATA 3 11 C0488 64 18 KT DATA DATA-ERR C0488 64 19 K9 CM3/S/MOL CM3/S/MOL C0488 64 20 2.000 1.45E+0 4.94E-1 C0488 64 21 2.500 1.05E+1 1.58E+0 C0488 64 22 3.000 4.65E+1 6.98E+0 C0488 64 23 3.500 1.51E+2 2.27E+1 C0488 64 24 4.000 3.92E+2 5.88E+1 C0488 64 25 4.500 8.65E+2 1.30E+2 C0488 64 26 5.000 1.67E+3 2.51E+2 C0488 64 27 5.500 2.92E+3 4.38E+2 C0488 64 28 6.000 4.69E+3 8.42E+2 C0488 64 29 6.500 7.03E+3 1.62E+3 C0488 64 30 7.000 9.96E+3 2.81E+3 C0488 64 31 ENDDATA 13 0 C0488 64 32 ENDSUBENT 31 0 C0488 6499999 SUBENT C0488065 20160323 C158C0488 65 1 BIB 5 13 C0488 65 2 REACTION (42-MO-92(P,G)43-TC-93-M,,SGV) C0488 65 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488 65 4 directly from measured reaction cross sections and C0488 65 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488 65 7 value of the product of the cross section times the C0488 65 8 velocity, averaged over the Maxwell-Boltzmann C0488 65 9 velocity distribution at the temperature T of interest.C0488 65 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488 65 11 their values were added quadratically. C0488 65 12 STATUS (TABLE) Table III, page 191. C0488 65 13 (DEP,C0487020) C0488 65 14 HISTORY (20160323C) BP C0488 65 15 ENDBIB 13 0 C0488 65 16 NOCOMMON 0 0 C0488 65 17 DATA 3 11 C0488 65 18 KT DATA DATA-ERR C0488 65 19 K9 CM3/S/MOL CM3/S/MOL C0488 65 20 2.000 6.21E-1 1.82E-1 C0488 65 21 2.500 4.50E+0 6.75E-1 C0488 65 22 3.000 1.95E+1 2.93E+0 C0488 65 23 3.500 6.14E+1 9.21E+0 C0488 65 24 4.000 1.55E+2 2.33E+1 C0488 65 25 4.500 3.36E+2 5.04E+1 C0488 65 26 5.000 6.40E+2 9.60E+1 C0488 65 27 5.500 1.11E+3 1.67E+2 C0488 65 28 6.000 1.77E+3 3.23E+2 C0488 65 29 6.500 2.64E+3 6.22E+2 C0488 65 30 7.000 3.74E+3 1.10E+3 C0488 65 31 ENDDATA 13 0 C0488 65 32 ENDSUBENT 31 0 C0488 6599999 SUBENT C0488066 20160323 C158C0488 66 1 BIB 5 13 C0488 66 2 REACTION (42-MO-95(P,G)43-TC-96,,SGV) C0488 66 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488 66 4 directly from measured reaction cross sections and C0488 66 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488 66 7 value of the product of the cross section times the C0488 66 8 velocity, averaged over the Maxwell-Boltzmann C0488 66 9 velocity distribution at the temperature T of interest.C0488 66 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488 66 11 their values were added quadratically. C0488 66 12 STATUS (TABLE) Table III, page 191. C0488 66 13 (DEP,C0487021) C0488 66 14 HISTORY (20160323C) BP C0488 66 15 ENDBIB 13 0 C0488 66 16 NOCOMMON 0 0 C0488 66 17 DATA 3 10 C0488 66 18 KT DATA DATA-ERR C0488 66 19 K9 CM3/S/MOL CM3/S/MOL C0488 66 20 2.500 4.42E+1 9.28E+0 C0488 66 21 3.000 1.90E+2 2.85E+1 C0488 66 22 3.500 5.65E+2 8.48E+1 C0488 66 23 4.000 1.31E+3 1.97E+2 C0488 66 24 4.500 2.56E+3 3.84E+2 C0488 66 25 5.000 4.39E+3 6.59E+2 C0488 66 26 5.500 6.86E+3 1.03E+3 C0488 66 27 6.000 9.96E+3 1.49E+3 C0488 66 28 6.500 1.36E+4 2.04E+3 C0488 66 29 7.000 1.78E+4 3.32E+3 C0488 66 30 ENDDATA 12 0 C0488 66 31 ENDSUBENT 30 0 C0488 6699999 SUBENT C0488067 20160323 C158C0488 67 1 BIB 5 13 C0488 67 2 REACTION (42-MO-95(P,G)43-TC-96-M,,SGV) C0488 67 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488 67 4 directly from measured reaction cross sections and C0488 67 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488 67 7 value of the product of the cross section times the C0488 67 8 velocity, averaged over the Maxwell-Boltzmann C0488 67 9 velocity distribution at the temperature T of interest.C0488 67 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488 67 11 their values were added quadratically. C0488 67 12 STATUS (TABLE) Table III, page 191. C0488 67 13 (DEP,C0487022) C0488 67 14 HISTORY (20160323C) BP C0488 67 15 ENDBIB 13 0 C0488 67 16 NOCOMMON 0 0 C0488 67 17 DATA 3 10 C0488 67 18 KT DATA DATA-ERR C0488 67 19 K9 CM3/S/MOL CM3/S/MOL C0488 67 20 2.500 1.75E+0 1.24E+0 C0488 67 21 3.000 7.97E+0 3.70E+0 C0488 67 22 3.500 2.35E+1 8.45E+0 C0488 67 23 4.000 5.29E+1 1.69E+1 C0488 67 24 4.500 9.87E+1 3.21E+1 C0488 67 25 5.000 1.62E+2 5.84E+1 C0488 67 26 5.800 2.40E+2 9.93E+1 C0488 67 27 6.000 3.32E+2 9.45E+1 C0488 67 28 6.500 4.34E+2 2.38E+2 C0488 67 29 7.000 5.42E+2 3.25E+2 C0488 67 30 ENDDATA 12 0 C0488 67 31 ENDSUBENT 30 0 C0488 6799999 SUBENT C0488068 20160323 C158C0488 68 1 BIB 5 13 C0488 68 2 REACTION (42-MO-98(P,G)43-TC-99-M,,SGV) C0488 68 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488 68 4 directly from measured reaction cross sections and C0488 68 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488 68 7 value of the product of the cross section times the C0488 68 8 velocity, averaged over the Maxwell-Boltzmann C0488 68 9 velocity distribution at the temperature T of interest.C0488 68 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488 68 11 their values were added quadratically. C0488 68 12 STATUS (TABLE) Table III, page 191. C0488 68 13 (DEP,C0487023) C0488 68 14 HISTORY (20160323C) BP C0488 68 15 ENDBIB 13 0 C0488 68 16 NOCOMMON 0 0 C0488 68 17 DATA 3 8 C0488 68 18 KT DATA DATA-ERR C0488 68 19 K9 CM3/S/MOL CM3/S/MOL C0488 68 20 1.500 1.85E+0 4.72E-1 C0488 68 21 2.000 5.47E+1 8.20E+0 C0488 68 22 2.500 4.68E+2 7.02E+1 C0488 68 23 3.000 2.02E+3 3.03E+2 C0488 68 24 3.500 5.82E+3 8.73E+2 C0488 68 25 4.000 1.29E+4 1.94E+3 C0488 68 26 4.500 2.36E+4 3.57E+3 C0488 68 27 5.000 3.90E+4 5.85E+3 C0488 68 28 ENDDATA 10 0 C0488 68 29 ENDSUBENT 28 0 C0488 6899999 SUBENT C0488069 20160323 C158C0488 69 1 BIB 5 13 C0488 69 2 REACTION (42-MO-100(P,G)43-TC-101,,SGV) C0488 69 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488 69 4 directly from measured reaction cross sections and C0488 69 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488 69 7 value of the product of the cross section times the C0488 69 8 velocity, averaged over the Maxwell-Boltzmann C0488 69 9 velocity distribution at the temperature T of interest.C0488 69 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488 69 11 their values were added quadratically. C0488 69 12 STATUS (TABLE) Table III, page 191. C0488 69 13 (DEP,C0487024) C0488 69 14 HISTORY (20160323C) BP C0488 69 15 ENDBIB 13 0 C0488 69 16 NOCOMMON 0 0 C0488 69 17 DATA 3 10 C0488 69 18 KT DATA DATA-ERR C0488 69 19 K9 CM3/S/MOL CM3/S/MOL C0488 69 20 2.500 3.64E-1 1.22E-1 C0488 69 21 3.000 1.86E+0 3.05E-1 C0488 69 22 3.500 6.83E+0 1.02E+0 C0488 69 23 4.000 1.99E+1 2.98E+0 C0488 69 24 4.500 4.80E+1 7.20E+0 C0488 69 25 5.000 1.00E+2 1.50E+1 C0488 69 26 5.500 1.85E+2 3.79E+1 C0488 69 27 6.000 3.12E+2 8.20E+1 C0488 69 28 6.500 4.87E+2 1.59E+2 C0488 69 29 7.000 7.12E+2 2.80E+2 C0488 69 30 ENDDATA 12 0 C0488 69 31 ENDSUBENT 30 0 C0488 6999999 SUBENT C0488070 20160323 C158C0488 70 1 BIB 5 13 C0488 70 2 REACTION (46-PD-102(P,G)47-AG-103,,SGV) C0488 70 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488 70 4 directly from measured reaction cross sections and C0488 70 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488 70 7 value of the product of the cross section times the C0488 70 8 velocity, averaged over the Maxwell-Boltzmann C0488 70 9 velocity distribution at the temperature T of interest.C0488 70 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488 70 11 their values were added quadratically. C0488 70 12 STATUS (TABLE) Table III, page 191. C0488 70 13 (DEP,C0488005) C0488 70 14 HISTORY (20160323C) BP C0488 70 15 ENDBIB 13 0 C0488 70 16 NOCOMMON 0 0 C0488 70 17 DATA 3 11 C0488 70 18 KT DATA DATA-ERR C0488 70 19 K9 CM3/S/MOL CM3/S/MOL C0488 70 20 3.000 7.87E+1 3.84E+1 C0488 70 21 3.500 3.19E+2 8.93E+1 C0488 70 22 4.000 1.00E+3 1.67E+2 C0488 70 23 4.500 2.62E+3 3.93E+2 C0488 70 24 5.000 5.98E+3 8.97E+2 C0488 70 25 5.500 1.22E+4 1.83E+3 C0488 70 26 6.000 2.28E+4 3.42E+3 C0488 70 27 6.500 3.94E+4 5.91E+3 C0488 70 28 7.000 6.36E+4 9.54E+3 C0488 70 29 7.500 9.73E+4 1.76E+4 C0488 70 30 8.000 1.42E+5 3.12E+4 C0488 70 31 ENDDATA 13 0 C0488 70 32 ENDSUBENT 31 0 C0488 7099999 SUBENT C0488071 20160323 C158C0488 71 1 BIB 5 13 C0488 71 2 REACTION (48-CD-106(P,G)49-IN-107,,SGV) C0488 71 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488 71 4 directly from measured reaction cross sections and C0488 71 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488 71 7 value of the product of the cross section times the C0488 71 8 velocity, averaged over the Maxwell-Boltzmann C0488 71 9 velocity distribution at the temperature T of interest.C0488 71 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488 71 11 their values were added quadratically. C0488 71 12 STATUS (TABLE) Table III, page 191. C0488 71 13 (DEP,C0488006) C0488 71 14 HISTORY (20160323C) BP C0488 71 15 ENDBIB 13 0 C0488 71 16 NOCOMMON 0 0 C0488 71 17 DATA 3 7 C0488 71 18 KT DATA DATA-ERR C0488 71 19 K9 CM3/S/MOL CM3/S/MOL C0488 71 20 4.000 4.12E+2 1.67E+2 C0488 71 21 4.500 1.06E+3 3.31E+2 C0488 71 22 5.000 2.31E+3 6.65E+2 C0488 71 23 5.500 4.43E+3 1.38E+3 C0488 71 24 6.000 7.70E+3 2.82E+3 C0488 71 25 6.500 1.23E+4 5.31E+3 C0488 71 26 7.000 1.85E+4 9.38E+3 C0488 71 27 ENDDATA 9 0 C0488 71 28 ENDSUBENT 27 0 C0488 7199999 SUBENT C0488072 20160323 C158C0488 72 1 BIB 5 13 C0488 72 2 REACTION (48-CD-108(P,G)49-IN-109,,SGV) C0488 72 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488 72 4 directly from measured reaction cross sections and C0488 72 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488 72 7 value of the product of the cross section times the C0488 72 8 velocity, averaged over the Maxwell-Boltzmann C0488 72 9 velocity distribution at the temperature T of interest.C0488 72 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488 72 11 their values were added quadratically. C0488 72 12 STATUS (TABLE) Table III, page 191. C0488 72 13 (DEP,C0488007) C0488 72 14 HISTORY (20160323C) BP C0488 72 15 ENDBIB 13 0 C0488 72 16 NOCOMMON 0 0 C0488 72 17 DATA 3 6 C0488 72 18 KT DATA DATA-ERR C0488 72 19 K9 CM3/S/MOL CM3/S/MOL C0488 72 20 4.000 8.01E+2 3.72E+2 C0488 72 21 4.500 2.05E+3 7.32E+2 C0488 72 22 5.000 4.47E+3 1.48E+3 C0488 72 23 5.500 8.62E+3 3.09E+3 C0488 72 24 6.000 1.50E+4 6.29E+3 C0488 72 25 6.500 2.42E+4 1.20E+4 C0488 72 26 ENDDATA 8 0 C0488 72 27 ENDSUBENT 26 0 C0488 7299999 SUBENT C0488073 20160323 C158C0488 73 1 BIB 5 13 C0488 73 2 REACTION (48-CD-114(P,G)49-IN-115-M,,SGV) C0488 73 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488 73 4 directly from measured reaction cross sections and C0488 73 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488 73 7 value of the product of the cross section times the C0488 73 8 velocity, averaged over the Maxwell-Boltzmann C0488 73 9 velocity distribution at the temperature T of interest.C0488 73 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488 73 11 their values were added quadratically. C0488 73 12 STATUS (TABLE) Table III, page 191. C0488 73 13 (DEP,C0488008) C0488 73 14 HISTORY (20160323C) BP C0488 73 15 ENDBIB 13 0 C0488 73 16 NOCOMMON 0 0 C0488 73 17 DATA 3 5 C0488 73 18 KT DATA DATA-ERR C0488 73 19 K9 CM3/S/MOL CM3/S/MOL C0488 73 20 6.000 1.23E+3 6.06E+2 C0488 73 21 6.500 1.78E+3 7.99E+2 C0488 73 22 7.000 2.45E+3 1.06E+3 C0488 73 23 7.500 3.23E+3 1.40E+3 C0488 73 24 8.000 4.12E+3 1.87E+3 C0488 73 25 ENDDATA 7 0 C0488 73 26 ENDSUBENT 25 0 C0488 7399999 SUBENT C0488074 20160323 C158C0488 74 1 BIB 5 13 C0488 74 2 REACTION (48-CD-116(P,G)49-IN-117-M,,SGV) C0488 74 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488 74 4 directly from measured reaction cross sections and C0488 74 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488 74 7 value of the product of the cross section times the C0488 74 8 velocity, averaged over the Maxwell-Boltzmann C0488 74 9 velocity distribution at the temperature T of interest.C0488 74 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488 74 11 their values were added quadratically. C0488 74 12 STATUS (TABLE) Table III, page 191. C0488 74 13 (DEP,C0488009) C0488 74 14 HISTORY (20160323C) BP C0488 74 15 ENDBIB 13 0 C0488 74 16 NOCOMMON 0 0 C0488 74 17 DATA 3 6 C0488 74 18 KT DATA DATA-ERR C0488 74 19 K9 CM3/S/MOL CM3/S/MOL C0488 74 20 3.500 2.38E+0 1.02E+0 C0488 74 21 4.000 7.94E+0 2.46E+0 C0488 74 22 4.500 2.11E+1 5.90E+0 C0488 74 23 5.000 4.76E+1 1.50E+1 C0488 74 24 5.500 9.40E+1 3.66E+1 C0488 74 25 6.000 1.67E+2 8.02E+1 C0488 74 26 ENDDATA 8 0 C0488 74 27 ENDSUBENT 26 0 C0488 7499999 SUBENT C0488075 20160324 C158C0488 75 1 BIB 5 13 C0488 75 2 REACTION (50-SN-112(P,G)51-SB-113,,SGV) C0488 75 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488 75 4 directly from measured reaction cross sections and C0488 75 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488 75 7 value of the product of the cross section times the C0488 75 8 velocity, averaged over the Maxwell-Boltzmann C0488 75 9 velocity distribution at the temperature T of interest.C0488 75 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488 75 11 their values were added quadratically. C0488 75 12 STATUS (TABLE) Table III, page 192. C0488 75 13 (DEP,C0488010) C0488 75 14 HISTORY (20160324C) BP C0488 75 15 ENDBIB 13 0 C0488 75 16 NOCOMMON 0 0 C0488 75 17 DATA 3 5 C0488 75 18 KT DATA DATA-ERR C0488 75 19 K9 CM3/S/MOL CM3/S/MOL C0488 75 20 3.500 2.29E+2 1.15E+2 C0488 75 21 4.000 6.90E+2 3.21E+2 C0488 75 22 4.500 1.62E+3 7.94E+2 C0488 75 23 5.000 3.20E+3 1.76E+3 C0488 75 24 5.500 5.54E+3 3.50E+3 C0488 75 25 ENDDATA 7 0 C0488 75 26 ENDSUBENT 25 0 C0488 7599999 SUBENT C0488076 20160324 C158C0488 76 1 BIB 5 13 C0488 76 2 REACTION (62-SM-144(P,G)63-EU-145,,SGV) C0488 76 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488 76 4 directly from measured reaction cross sections and C0488 76 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488 76 7 value of the product of the cross section times the C0488 76 8 velocity, averaged over the Maxwell-Boltzmann C0488 76 9 velocity distribution at the temperature T of interest.C0488 76 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488 76 11 their values were added quadratically. C0488 76 12 STATUS (TABLE) Table III, page 192. C0488 76 13 (DEP,C0488011) C0488 76 14 HISTORY (20160324C) BP C0488 76 15 ENDBIB 13 0 C0488 76 16 NOCOMMON 0 0 C0488 76 17 DATA 3 10 C0488 76 18 KT DATA DATA-ERR C0488 76 19 K9 CM3/S/MOL CM3/S/MOL C0488 76 20 3.500 2.70E+1 1.34E+1 C0488 76 21 4.000 9.06E+1 3.35E+1 C0488 76 22 4.500 2.41E+2 6.92E+1 C0488 76 23 5.000 5.50E+2 1.10E+2 C0488 76 24 5.500 1.13E+3 1.85E+2 C0488 76 25 6.000 2.14E+3 3.45E+2 C0488 76 26 6.500 3.79E+3 7.19E+2 C0488 76 27 7.000 6.31E+3 1.49E+3 C0488 76 28 7.500 9.96E+3 2.93E+3 C0488 76 29 8.000 1.50E+4 5.34E+3 C0488 76 30 ENDDATA 12 0 C0488 76 31 ENDSUBENT 30 0 C0488 7699999 SUBENT C0488077 20160324 C158C0488 77 1 BIB 5 13 C0488 77 2 REACTION (30-ZN-68(P,N)31-GA-68,,SGV) C0488 77 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488 77 4 directly from measured reaction cross sections and C0488 77 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488 77 7 value of the product of the cross section times the C0488 77 8 velocity, averaged over the Maxwell-Boltzmann C0488 77 9 velocity distribution at the temperature T of interest.C0488 77 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488 77 11 their values were added quadratically. C0488 77 12 STATUS (TABLE) Table III, page 192. C0488 77 13 (DEP,C0487025) C0488 77 14 HISTORY (20160324C) BP C0488 77 15 ENDBIB 13 0 C0488 77 16 NOCOMMON 0 0 C0488 77 17 DATA 3 5 C0488 77 18 KT DATA DATA-ERR C0488 77 19 K9 CM3/S/MOL CM3/S/MOL C0488 77 20 3.000 1.63E+2 2.55E+1 C0488 77 21 3.500 1.34E+3 2.71E+2 C0488 77 22 4.000 6.47E+3 1.74E+3 C0488 77 23 4.500 2.18E+4 7.55E+3 C0488 77 24 5.000 5.65E+4 2.45E+4 C0488 77 25 ENDDATA 7 0 C0488 77 26 ENDSUBENT 25 0 C0488 7799999 SUBENT C0488078 20160324 C158C0488 78 1 BIB 5 13 C0488 78 2 REACTION (32-GE-74(P,N)33-AS-74,,SGV) C0488 78 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488 78 4 directly from measured reaction cross sections and C0488 78 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488 78 7 value of the product of the cross section times the C0488 78 8 velocity, averaged over the Maxwell-Boltzmann C0488 78 9 velocity distribution at the temperature T of interest.C0488 78 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488 78 11 their values were added quadratically. C0488 78 12 STATUS (TABLE) Table III, page 192. C0488 78 13 (DEP,C0487026) C0488 78 14 HISTORY (20160324C) BP C0488 78 15 ENDBIB 13 0 C0488 78 16 NOCOMMON 0 0 C0488 78 17 DATA 3 10 C0488 78 18 KT DATA DATA-ERR C0488 78 19 K9 CM3/S/MOL CM3/S/MOL C0488 78 20 2.500 3.61E+1 5.41E+0 C0488 78 21 3.000 5.28E+2 7.92E+1 C0488 78 22 3.500 3.61E+3 5.42E+2 C0488 78 23 4.000 1.53E+4 2.30E+3 C0488 78 24 4.500 4.67E+4 7.75E+3 C0488 78 25 5.000 1.13E+5 2.50E+4 C0488 78 26 5.500 2.33E+5 6.52E+4 C0488 78 27 6.000 4.22E+5 1.44E+5 C0488 78 28 6.500 6.92E+5 2.82E+5 C0488 78 29 7.000 1.05E+6 4.96E+6 C0488 78 30 ENDDATA 12 0 C0488 78 31 ENDSUBENT 30 0 C0488 7899999 SUBENT C0488079 20160324 C158C0488 79 1 BIB 5 13 C0488 79 2 REACTION (32-GE-76(P,N)33-AS-76,,SGV) C0488 79 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488 79 4 directly from measured reaction cross sections and C0488 79 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488 79 7 value of the product of the cross section times the C0488 79 8 velocity, averaged over the Maxwell-Boltzmann C0488 79 9 velocity distribution at the temperature T of interest.C0488 79 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488 79 11 their values were added quadratically. C0488 79 12 STATUS (TABLE) Table III, page 192. C0488 79 13 (DEP,C0487027) C0488 79 14 HISTORY (20160324C) BP C0488 79 15 ENDBIB 13 0 C0488 79 16 NOCOMMON 0 0 C0488 79 17 DATA 3 11 C0488 79 18 KT DATA DATA-ERR C0488 79 19 K9 CM3/S/MOL CM3/S/MOL C0488 79 20 2.000 9.04E+1 2.29E+1 C0488 79 21 2.500 1.10E+3 1.65E+2 C0488 79 22 3.000 6.35E+3 9.53E+2 C0488 79 23 3.500 2.40E+4 3.60E+3 C0488 79 24 4.000 6.86E+4 1.03E+4 C0488 79 25 4.500 1.61E+5 2.42E+4 C0488 79 26 5.000 3.26E+5 4.89E+4 C0488 79 27 5.500 5.87E+5 9.59E+4 C0488 79 28 6.000 9.66E+5 2.05E+5 C0488 79 29 6.500 1.45E+6 3.94E+5 C0488 79 30 7.000 2.13E+6 6.91E+5 C0488 79 31 ENDDATA 13 0 C0488 79 32 ENDSUBENT 31 0 C0488 7999999 SUBENT C0488080 20160324 C158C0488 80 1 BIB 5 13 C0488 80 2 REACTION (38-SR-87(P,N)39-Y-87,,SGV) C0488 80 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488 80 4 directly from measured reaction cross sections and C0488 80 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488 80 7 value of the product of the cross section times the C0488 80 8 velocity, averaged over the Maxwell-Boltzmann C0488 80 9 velocity distribution at the temperature T of interest.C0488 80 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488 80 11 their values were added quadratically. C0488 80 12 STATUS (TABLE) Table III, page 192. C0488 80 13 (DEP,C0488012) C0488 80 14 HISTORY (20160324C) BP C0488 80 15 ENDBIB 13 0 C0488 80 16 NOCOMMON 0 0 C0488 80 17 DATA 3 11 C0488 80 18 KT DATA DATA-ERR C0488 80 19 K9 CM3/S/MOL CM3/S/MOL C0488 80 20 3.000 3.84E+2 5.76E+1 C0488 80 21 3.500 1.75E+3 2.63E+2 C0488 80 22 4.000 5.81E+3 8.72E+2 C0488 80 23 4.500 1.55E+4 2.33E+3 C0488 80 24 5.000 3.50E+4 5.25E+3 C0488 80 25 5.500 6.93E+4 1.04E+4 C0488 80 26 6.000 1.24E+5 1.86E+4 C0488 80 27 6.500 2.03E+5 3.82E+4 C0488 80 28 7.000 3.12E+5 7.33E+4 C0488 80 29 7.500 4.53E+5 1.29E+5 C0488 80 30 8.000 6.27E+5 2.11E+5 C0488 80 31 ENDDATA 13 0 C0488 80 32 ENDSUBENT 31 0 C0488 8099999 SUBENT C0488081 20160324 C158C0488 81 1 BIB 5 13 C0488 81 2 REACTION (38-SR-88(P,N)39-Y-88,,SGV) C0488 81 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488 81 4 directly from measured reaction cross sections and C0488 81 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488 81 7 value of the product of the cross section times the C0488 81 8 velocity, averaged over the Maxwell-Boltzmann C0488 81 9 velocity distribution at the temperature T of interest.C0488 81 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488 81 11 their values were added quadratically. C0488 81 12 STATUS (TABLE) Table III, page 192. C0488 81 13 (DEP,C0488013) C0488 81 14 HISTORY (20160324C) BP C0488 81 15 ENDBIB 13 0 C0488 81 16 NOCOMMON 0 0 C0488 81 17 DATA 3 5 C0488 81 18 KT DATA DATA-ERR C0488 81 19 K9 CM3/S/MOL CM3/S/MOL C0488 81 20 2.000 1.86E-3 2.79E-4 C0488 81 21 2.500 4.25E-1 6.76E-2 C0488 81 22 3.000 1.61E+1 4.67E+0 C0488 81 23 3.500 2.18E+2 9.68E+1 C0488 81 24 4.000 1.53E+3 9.38E+2 C0488 81 25 ENDDATA 7 0 C0488 81 26 ENDSUBENT 25 0 C0488 8199999 SUBENT C0488082 20160324 C158C0488 82 1 BIB 5 13 C0488 82 2 REACTION (40-ZR-94(P,N)41-NB-94-M,,SGV) C0488 82 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488 82 4 directly from measured reaction cross sections and C0488 82 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488 82 7 value of the product of the cross section times the C0488 82 8 velocity, averaged over the Maxwell-Boltzmann C0488 82 9 velocity distribution at the temperature T of interest.C0488 82 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488 82 11 their values were added quadratically. C0488 82 12 STATUS (TABLE) Table III, page 192. C0488 82 13 (DEP,C0488014) C0488 82 14 HISTORY (20160324C) BP C0488 82 15 ENDBIB 13 0 C0488 82 16 NOCOMMON 0 0 C0488 82 17 DATA 3 10 C0488 82 18 KT DATA DATA-ERR C0488 82 19 K9 CM3/S/MOL CM3/S/MOL C0488 82 20 3.500 6.37E+3 2.01E+3 C0488 82 21 4.000 2.21E+4 4.94E+3 C0488 82 22 4.500 6.06E+4 9.09E+3 C0488 82 23 5.000 1.40E+5 2.10E+4 C0488 82 24 5.500 2.85E+5 4.28E+4 C0488 82 25 6.000 5.21E+5 7.82E+4 C0488 82 26 6.500 8.77E+5 1.66E+5 C0488 82 27 7.000 1.30E+6 3.24E+5 C0488 82 28 7.500 2.04E+6 6.34E+5 C0488 82 29 8.000 2.88E+6 1.03E+6 C0488 82 30 ENDDATA 12 0 C0488 82 31 ENDSUBENT 30 0 C0488 8299999 SUBENT C0488083 20160324 C158C0488 83 1 BIB 5 13 C0488 83 2 REACTION (40-ZR-96(P,N)41-NB-96,,SGV) C0488 83 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488 83 4 directly from measured reaction cross sections and C0488 83 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488 83 7 value of the product of the cross section times the C0488 83 8 velocity, averaged over the Maxwell-Boltzmann C0488 83 9 velocity distribution at the temperature T of interest.C0488 83 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488 83 11 their values were added quadratically. C0488 83 12 STATUS (TABLE) Table III, page 192. C0488 83 13 (DEP,C0488015) C0488 83 14 HISTORY (20160324C) BP C0488 83 15 ENDBIB 13 0 C0488 83 16 NOCOMMON 0 0 C0488 83 17 DATA 3 10 C0488 83 18 KT DATA DATA-ERR C0488 83 19 K9 CM3/S/MOL CM3/S/MOL C0488 83 20 3.500 2.36E+3 9.92E+2 C0488 83 21 4.000 8.21E+3 2.39E+3 C0488 83 22 4.500 2.28E+4 4.21E+3 C0488 83 23 5.000 5.37E+4 1.14E+4 C0488 83 24 5.500 1.11E+5 1.76E+4 C0488 83 25 6.000 2.07E+5 4.01E+4 C0488 83 26 6.500 3.55E+5 8.64E+4 C0488 83 27 7.000 5.66E+5 1.70E+5 C0488 83 28 7.500 8.50E+5 3.34E+5 C0488 83 29 8.000 1.22E+6 5.50E+5 C0488 83 30 ENDDATA 12 0 C0488 83 31 ENDSUBENT 30 0 C0488 8399999 SUBENT C0488084 20160324 C158C0488 84 1 BIB 5 13 C0488 84 2 REACTION (42-MO-95(P,N)43-TC-95,,SGV) C0488 84 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488 84 4 directly from measured reaction cross sections and C0488 84 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488 84 7 value of the product of the cross section times the C0488 84 8 velocity, averaged over the Maxwell-Boltzmann C0488 84 9 velocity distribution at the temperature T of interest.C0488 84 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488 84 11 their values were added quadratically. C0488 84 12 STATUS (TABLE) Table III, page 192. C0488 84 13 (DEP,C0487028) C0488 84 14 HISTORY (20160324C) BP C0488 84 15 ENDBIB 13 0 C0488 84 16 NOCOMMON 0 0 C0488 84 17 DATA 3 7 C0488 84 18 KT DATA DATA-ERR C0488 84 19 K9 CM3/S/MOL CM3/S/MOL C0488 84 20 2.500 1.04E+1 4.50E+0 C0488 84 21 3.000 1.03E+2 2.77E+1 C0488 84 22 3.500 5.49E+2 1.20E+2 C0488 84 23 4.000 1.98E+3 4.60E+2 C0488 84 24 4.500 5.45E+3 1.59E+3 C0488 84 25 5.000 1.23E+4 4.57E+3 C0488 84 26 5.500 2.40E+4 1.11E+4 C0488 84 27 ENDDATA 9 0 C0488 84 28 ENDSUBENT 27 0 C0488 8499999 SUBENT C0488085 20160324 C158C0488 85 1 BIB 5 13 C0488 85 2 REACTION (42-MO-95(P,N)43-TC-95-M,,SGV) C0488 85 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488 85 4 directly from measured reaction cross sections and C0488 85 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488 85 7 value of the product of the cross section times the C0488 85 8 velocity, averaged over the Maxwell-Boltzmann C0488 85 9 velocity distribution at the temperature T of interest.C0488 85 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488 85 11 their values were added quadratically. C0488 85 12 STATUS (TABLE) Table III, page 192. C0488 85 13 (DEP,C0487029) C0488 85 14 HISTORY (20160324C) BP C0488 85 15 ENDBIB 13 0 C0488 85 16 NOCOMMON 0 0 C0488 85 17 DATA 3 6 C0488 85 18 KT DATA DATA-ERR C0488 85 19 K9 CM3/S/MOL CM3/S/MOL C0488 85 20 2.500 2.12E+1 8.55E+0 C0488 85 21 3.000 2.20E+2 6.50E+1 C0488 85 22 3.500 1.19E+3 3.20E+2 C0488 85 23 4.000 4.27E+3 1.32E+3 C0488 85 24 4.500 1.16E+4 4.48E+3 C0488 85 25 5.000 2.57E+4 1.25E+4 C0488 85 26 ENDDATA 8 0 C0488 85 27 ENDSUBENT 26 0 C0488 8599999 SUBENT C0488086 20160324 C158C0488 86 1 BIB 5 13 C0488 86 2 REACTION (42-MO-96(P,N)43-TC-96,,SGV) C0488 86 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488 86 4 directly from measured reaction cross sections and C0488 86 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488 86 7 value of the product of the cross section times the C0488 86 8 velocity, averaged over the Maxwell-Boltzmann C0488 86 9 velocity distribution at the temperature T of interest.C0488 86 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488 86 11 their values were added quadratically. C0488 86 12 STATUS (TABLE) Table III, page 192. C0488 86 13 (DEP,C0487030) C0488 86 14 HISTORY (20160324C) BP C0488 86 15 ENDBIB 13 0 C0488 86 16 NOCOMMON 0 0 C0488 86 17 DATA 3 10 C0488 86 18 KT DATA DATA-ERR C0488 86 19 K9 CM3/S/MOL CM3/S/MOL C0488 86 20 2.000 1.83E-2 2.74E-3 C0488 86 21 2.500 1.58E+0 2.37E-1 C0488 86 22 3.000 3.14E+1 4.71E+0 C0488 86 23 3.500 2.65E+2 5.67E+1 C0488 86 24 4.000 1.30E+3 3.90E+2 C0488 86 25 4.500 4.46E+3 1.75E+3 C0488 86 26 5.000 1.18E+4 5.77E+3 C0488 86 27 5.500 2.59E+4 1.53E+4 C0488 86 28 6.000 4.96E+4 3.43E+4 C0488 86 29 6.500 8.52E+4 6.78E+4 C0488 86 30 ENDDATA 12 0 C0488 86 31 ENDSUBENT 30 0 C0488 8699999 SUBENT C0488087 20160324 C158C0488 87 1 BIB 5 13 C0488 87 2 REACTION (42-MO-96(P,N)43-TC-96-M,,SGV) C0488 87 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488 87 4 directly from measured reaction cross sections and C0488 87 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488 87 7 value of the product of the cross section times the C0488 87 8 velocity, averaged over the Maxwell-Boltzmann C0488 87 9 velocity distribution at the temperature T of interest.C0488 87 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488 87 11 their values were added quadratically. C0488 87 12 STATUS (TABLE) Table III, page 192. C0488 87 13 (DEP,C0487031) C0488 87 14 HISTORY (20160324C) BP C0488 87 15 ENDBIB 13 0 C0488 87 16 NOCOMMON 0 0 C0488 87 17 DATA 3 7 C0488 87 18 KT DATA DATA-ERR C0488 87 19 K9 CM3/S/MOL CM3/S/MOL C0488 87 20 2.000 8.46E-3 1.27E-3 C0488 87 21 2.500 7.51E-1 1.13E-1 C0488 87 22 3.000 1.51E-1 2.27E+0 C0488 87 23 3.500 1.28E+2 2.66E+1 C0488 87 24 4.000 6.34E+2 1.85E+2 C0488 87 25 4.500 2.17E+3 8.27E+2 C0488 87 26 5.000 5.75E+3 2.72E+3 C0488 87 27 ENDDATA 9 0 C0488 87 28 ENDSUBENT 27 0 C0488 8799999 SUBENT C0488088 20160324 C158C0488 88 1 BIB 5 13 C0488 88 2 REACTION (46-PD-104(P,N)47-AG-104,,SGV) C0488 88 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488 88 4 directly from measured reaction cross sections and C0488 88 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488 88 7 value of the product of the cross section times the C0488 88 8 velocity, averaged over the Maxwell-Boltzmann C0488 88 9 velocity distribution at the temperature T of interest.C0488 88 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488 88 11 their values were added quadratically. C0488 88 12 STATUS (TABLE) Table III, page 192. C0488 88 13 (DEP,C0488016) C0488 88 14 HISTORY (20160324C) BP C0488 88 15 ENDBIB 13 0 C0488 88 16 NOCOMMON 0 0 C0488 88 17 DATA 3 5 C0488 88 18 KT DATA DATA-ERR C0488 88 19 K9 CM3/S/MOL CM3/S/MOL C0488 88 20 2.000 1.48E-5 2.22E-6 C0488 88 21 2.500 6.01E-3 1.11E-3 C0488 88 22 3.000 3.24E-1 9.56E-2 C0488 88 23 3.500 5.50E+0 2.28E+0 C0488 88 24 4.000 4.51E+1 2.44E+1 C0488 88 25 ENDDATA 7 0 C0488 88 26 ENDSUBENT 25 0 C0488 8899999 SUBENT C0488089 20160324 C158C0488 89 1 BIB 5 13 C0488 89 2 REACTION (46-PD-105(P,N)47-AG-105,,SGV) C0488 89 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488 89 4 directly from measured reaction cross sections and C0488 89 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488 89 7 value of the product of the cross section times the C0488 89 8 velocity, averaged over the Maxwell-Boltzmann C0488 89 9 velocity distribution at the temperature T of interest.C0488 89 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488 89 11 their values were added quadratically. C0488 89 12 STATUS (TABLE) Table III, page 192. C0488 89 13 (DEP,C0488017) C0488 89 14 HISTORY (20160324C) BP C0488 89 15 ENDBIB 13 0 C0488 89 16 NOCOMMON 0 0 C0488 89 17 DATA 3 11 C0488 89 18 KT DATA DATA-ERR C0488 89 19 K9 CM3/S/MOL CM3/S/MOL C0488 89 20 3.000 6.59E+1 2.60E+1 C0488 89 21 3.500 4.37E+2 1.18E+2 C0488 89 22 4.000 1.89E+3 3.27E+2 C0488 89 23 4.500 6.09E+3 9.14E+2 C0488 89 24 5.000 1.59E+4 2.39E+3 C0488 89 25 5.500 3.53E+4 6.06E+3 C0488 89 26 6.000 6.90E+4 1.50E+4 C0488 89 27 6.500 1.22E+5 3.29E+4 C0488 89 28 7.000 2.00E+5 7.17E+4 C0488 89 29 7.500 3.06E+5 1.27E+5 C0488 89 30 8.000 4.44E+5 2.10E+5 C0488 89 31 ENDDATA 13 0 C0488 89 32 ENDSUBENT 31 0 C0488 8999999 SUBENT C0488090 20160324 C158C0488 90 1 BIB 5 13 C0488 90 2 REACTION (46-PD-106(P,N)47-AG-106,,SGV) C0488 90 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488 90 4 directly from measured reaction cross sections and C0488 90 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488 90 7 value of the product of the cross section times the C0488 90 8 velocity, averaged over the Maxwell-Boltzmann C0488 90 9 velocity distribution at the temperature T of interest.C0488 90 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488 90 11 their values were added quadratically. C0488 90 12 STATUS (TABLE) Table III, page 192. C0488 90 13 (DEP,C0488018) C0488 90 14 HISTORY (20160324C) BP C0488 90 15 ENDBIB 13 0 C0488 90 16 NOCOMMON 0 0 C0488 90 17 DATA 3 11 C0488 90 18 KT DATA DATA-ERR C0488 90 19 K9 CM3/S/MOL CM3/S/MOL C0488 90 20 2.500 2.87E+0 4.31E-1 C0488 90 21 3.000 5.99E+1 8.99E+0 C0488 90 22 3.500 5.56E+2 8.34E+1 C0488 90 23 4.000 3.05E+3 4.58E+2 C0488 90 24 4.500 1.17E+4 1.76E+3 C0488 90 25 5.000 3.43E+4 6.04E+3 C0488 90 26 5.500 8.32E+4 1.95E+4 C0488 90 27 6.000 1.74E+5 5.13E+4 C0488 90 28 6.500 3.23E+5 1.16E+5 C0488 90 29 7.000 5.49E+5 2.35E+5 C0488 90 30 7.500 8.66E+5 4.30E+5 C0488 90 31 ENDDATA 13 0 C0488 90 32 ENDSUBENT 31 0 C0488 9099999 SUBENT C0488091 20160324 C158C0488 91 1 BIB 5 13 C0488 91 2 REACTION (46-PD-106(P,N)47-AG-106-M,,SGV) C0488 91 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488 91 4 directly from measured reaction cross sections and C0488 91 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488 91 7 value of the product of the cross section times the C0488 91 8 velocity, averaged over the Maxwell-Boltzmann C0488 91 9 velocity distribution at the temperature T of interest.C0488 91 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488 91 11 their values were added quadratically. C0488 91 12 STATUS (TABLE) Table III, page 192. C0488 91 13 (DEP,C0488019) C0488 91 14 HISTORY (20160324C) BP C0488 91 15 ENDBIB 13 0 C0488 91 16 NOCOMMON 0 0 C0488 91 17 DATA 3 12 C0488 91 18 KT DATA DATA-ERR C0488 91 19 K9 CM3/S/MOL CM3/S/MOL C0488 91 20 2.500 4.84E-2 7.26E-3 C0488 91 21 3.000 8.80E-1 1.32E-1 C0488 91 22 3.500 7.09E+0 1.06E+0 C0488 91 23 4.000 3.44E+1 5.16E+0 C0488 91 24 4.500 1.19E+2 1.79E+1 C0488 91 25 5.000 3.23E+2 4.85E+1 C0488 91 26 5.500 7.34E+2 1.17E+2 C0488 91 27 6.000 1.46E+3 3.05E+2 C0488 91 28 6.500 2.60E+3 6.82E+2 C0488 91 29 7.000 4.28E+3 1.36E+3 C0488 91 30 7.500 6.57E+3 2.49E+3 C0488 91 31 8.000 9.54E+3 4.21E+3 C0488 91 32 ENDDATA 14 0 C0488 91 33 ENDSUBENT 32 0 C0488 9199999 SUBENT C0488092 20160324 C158C0488 92 1 BIB 5 13 C0488 92 2 REACTION (48-CD-116(P,N)49-IN-116-M,,SGV) C0488 92 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488 92 4 directly from measured reaction cross sections and C0488 92 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488 92 7 value of the product of the cross section times the C0488 92 8 velocity, averaged over the Maxwell-Boltzmann C0488 92 9 velocity distribution at the temperature T of interest.C0488 92 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488 92 11 their values were added quadratically. C0488 92 12 STATUS (TABLE) Table III, page 193. C0488 92 13 (DEP,C0488020) C0488 92 14 HISTORY (20160324C) BP C0488 92 15 ENDBIB 13 0 C0488 92 16 NOCOMMON 0 0 C0488 92 17 DATA 3 7 C0488 92 18 KT DATA DATA-ERR C0488 92 19 KEV CM3/S/MOL CM3/S/MOL C0488 92 20 2.500 1.54E+0 6.77E-1 C0488 92 21 3.000 1.51E+1 3.54E+0 C0488 92 22 3.500 8.62E+1 1.43E+1 C0488 92 23 4.000 3.40E+2 6.61E+1 C0488 92 24 4.500 1.03E+3 2.79E+2 C0488 92 25 5.000 2.53E+3 1.02E+3 C0488 92 26 5.500 5.33E+3 2.64E+3 C0488 92 27 ENDDATA 9 0 C0488 92 28 ENDSUBENT 27 0 C0488 9299999 SUBENT C0488093 20160324 C158C0488 93 1 BIB 5 13 C0488 93 2 REACTION (50-SN-115(P,N)51-SB-115,,SGV) C0488 93 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488 93 4 directly from measured reaction cross sections and C0488 93 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488 93 7 value of the product of the cross section times the C0488 93 8 velocity, averaged over the Maxwell-Boltzmann C0488 93 9 velocity distribution at the temperature T of interest.C0488 93 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488 93 11 their values were added quadratically. C0488 93 12 STATUS (TABLE) Table III, page 193. C0488 93 13 (DEP,C0488021) C0488 93 14 HISTORY (20160324C) BP C0488 93 15 ENDBIB 13 0 C0488 93 16 NOCOMMON 0 0 C0488 93 17 DATA 3 7 C0488 93 18 KT DATA DATA-ERR C0488 93 19 KEV CM3/S/MOL CM3/S/MOL C0488 93 20 2.500 1.22E-1 6.14E-2 C0488 93 21 3.000 3.70E+0 1.23E+0 C0488 93 22 3.500 4.34E+1 1.24E+1 C0488 93 23 4.000 2.76E+2 8.60E+1 C0488 93 24 4.500 1.17E+3 4.44E+2 C0488 93 25 5.000 3.73E+3 1.75E+3 C0488 93 26 5.500 9.59E+3 5.45E+3 C0488 93 27 ENDDATA 9 0 C0488 93 28 ENDSUBENT 27 0 C0488 9399999 SUBENT C0488094 20160324 C158C0488 94 1 BIB 5 13 C0488 94 2 REACTION (50-SN-117(P,N)51-SB-117,,SGV) C0488 94 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488 94 4 directly from measured reaction cross sections and C0488 94 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488 94 7 value of the product of the cross section times the C0488 94 8 velocity, averaged over the Maxwell-Boltzmann C0488 94 9 velocity distribution at the temperature T of interest.C0488 94 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488 94 11 their values were added quadratically. C0488 94 12 STATUS (TABLE) Table III, page 193. C0488 94 13 (DEP,C0488022) C0488 94 14 HISTORY (20160324C) BP C0488 94 15 ENDBIB 13 0 C0488 94 16 NOCOMMON 0 0 C0488 94 17 DATA 3 13 C0488 94 18 KT DATA DATA-ERR C0488 94 19 K9 CM3/S/MOL CM3/S/MOL C0488 94 20 1.500 8.04E-4 3.41E-4 C0488 94 21 2.000 1.76E-1 3.85E-2 C0488 94 22 2.500 5.11E+0 7.67E-1 C0488 94 23 3.000 5.56E+1 8.34E+0 C0488 94 24 3.500 3.46E+2 5.19E+1 C0488 94 25 4.000 1.49E+3 2.24E+2 C0488 94 26 4.500 4.91E+3 7.37E+2 C0488 94 27 5.000 1.34E+4 2.16E+3 C0488 94 28 5.500 3.03E+4 6.86E+3 C0488 94 29 6.000 6.11E+4 1.80E+4 C0488 94 30 6.500 1.11E+5 4.10E+4 C0488 94 31 7.000 1.88E+5 8.34E+4 C0488 94 32 7.500 2.90E+5 1.53E+5 C0488 94 33 ENDDATA 15 0 C0488 94 34 ENDSUBENT 33 0 C0488 9499999 SUBENT C0488095 20160324 C158C0488 95 1 BIB 5 13 C0488 95 2 REACTION (50-SN-120(P,N)51-SB-120,,SGV) C0488 95 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488 95 4 directly from measured reaction cross sections and C0488 95 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488 95 7 value of the product of the cross section times the C0488 95 8 velocity, averaged over the Maxwell-Boltzmann C0488 95 9 velocity distribution at the temperature T of interest.C0488 95 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488 95 11 their values were added quadratically. C0488 95 12 STATUS (TABLE) Table III, page 193. C0488 95 13 (DEP,C0488023) C0488 95 14 HISTORY (20160324C) BP C0488 95 15 ENDBIB 13 0 C0488 95 16 NOCOMMON 0 0 C0488 95 17 DATA 3 12 C0488 95 18 KT DATA DATA-ERR C0488 95 19 K9 CM3/S/MOL CM3/S/MOL C0488 95 20 2.500 1.14E+0 1.68E-1 C0488 95 21 3.000 2.03E+1 3.05E+0 C0488 95 22 3.500 1.70E+2 2.55E+1 C0488 95 23 4.000 8.67E+2 1.30E+2 C0488 95 24 4.500 3.13E+3 4.70E+2 C0488 95 25 5.000 8.80E+3 1.32E+3 C0488 95 26 5.500 2.06E+4 3.50E+3 C0488 95 27 6.000 4.17E+4 9.13E+3 C0488 95 28 6.500 7.59E+4 2.06E+4 C0488 95 29 7.000 1.26E+5 4.12E+4 C0488 95 30 7.500 1.90E+5 7.55E+4 C0488 95 31 8.000 2.87E+5 1.27E+5 C0488 95 32 ENDDATA 14 0 C0488 95 33 ENDSUBENT 32 0 C0488 9599999 SUBENT C0488096 20160324 C158C0488 96 1 BIB 5 13 C0488 96 2 REACTION (50-SN-122(P,N)51-SB-122,,SGV) C0488 96 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488 96 4 directly from measured reaction cross sections and C0488 96 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488 96 7 value of the product of the cross section times the C0488 96 8 velocity, averaged over the Maxwell-Boltzmann C0488 96 9 velocity distribution at the temperature T of interest.C0488 96 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488 96 11 their values were added quadratically. C0488 96 12 STATUS (TABLE) Table III, page 193. C0488 96 13 (DEP,C0488024) C0488 96 14 HISTORY (20160324C) BP C0488 96 15 ENDBIB 13 0 C0488 96 16 NOCOMMON 0 0 C0488 96 17 DATA 3 7 C0488 96 18 KT DATA DATA-ERR C0488 96 19 K9 CM3/S/MOL CM3/S/MOL C0488 96 20 4.000 9.90E+2 1.49E+2 C0488 96 21 4.500 3.35E+3 5.03E+2 C0488 96 22 5.000 9.07E+3 1.56E+3 C0488 96 23 5.500 2.00E+4 4.69E+3 C0488 96 24 6.000 4.19E+4 1.12E+4 C0488 96 25 6.500 7.62E+4 2.96E+4 C0488 96 26 7.000 1.27E+4 5.78E+4 C0488 96 27 ENDDATA 9 0 C0488 96 28 ENDSUBENT 27 0 C0488 9699999 SUBENT C0488097 20160324 C158C0488 97 1 BIB 5 13 C0488 97 2 REACTION (50-SN-124(P,N)51-SB-124,,SGV) C0488 97 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488 97 4 directly from measured reaction cross sections and C0488 97 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488 97 7 value of the product of the cross section times the C0488 97 8 velocity, averaged over the Maxwell-Boltzmann C0488 97 9 velocity distribution at the temperature T of interest.C0488 97 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488 97 11 their values were added quadratically. C0488 97 12 STATUS (TABLE) Table III, page 193. C0488 97 13 (DEP,C0488025) C0488 97 14 HISTORY (20160324C) BP C0488 97 15 ENDBIB 13 0 C0488 97 16 NOCOMMON 0 0 C0488 97 17 DATA 3 9 C0488 97 18 KT DATA DATA-ERR C0488 97 19 K9 CM3/S/MOL CM3/S/MOL C0488 97 20 4.000 1.64E+3 1.13E+3 C0488 97 21 4.500 5.21E+3 2.58E+3 C0488 97 22 5.000 1.35E+4 5.49E+3 C0488 97 23 5.500 2.97E+4 1.09E+4 C0488 97 24 6.000 5.77E+4 2.11E+4 C0488 97 25 6.500 1.02E+5 4.00E+4 C0488 97 26 7.000 1.66E+5 7.29E+4 C0488 97 27 7.500 2.53E+5 1.26E+5 C0488 97 28 8.000 3.66E+5 2.06E+5 C0488 97 29 ENDDATA 11 0 C0488 97 30 ENDSUBENT 29 0 C0488 9799999 SUBENT C0488098 20160324 C158C0488 98 1 BIB 5 13 C0488 98 2 REACTION (52-TE-123(P,N)53-I-123,,SGV) C0488 98 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488 98 4 directly from measured reaction cross sections and C0488 98 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488 98 7 value of the product of the cross section times the C0488 98 8 velocity, averaged over the Maxwell-Boltzmann C0488 98 9 velocity distribution at the temperature T of interest.C0488 98 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488 98 11 their values were added quadratically. C0488 98 12 STATUS (TABLE) Table III, page 193. C0488 98 13 (DEP,C0488026) C0488 98 14 HISTORY (20160324C) BP C0488 98 15 ENDBIB 13 0 C0488 98 16 NOCOMMON 0 0 C0488 98 17 DATA 3 12 C0488 98 18 KT DATA DATA-ERR C0488 98 19 K9 CM3/S/MOL CM3/S/MOL C0488 98 20 2.500 4.60E+0 9.61E-1 C0488 98 21 3.000 5.67E+1 8.50E+0 C0488 98 22 3.500 3.83E+2 5.75E+1 C0488 98 23 4.000 1.72E+3 2.58E+2 C0488 98 24 4.500 5.72E+3 8.58E+2 C0488 98 25 5.000 1.53E+4 2.30E+3 C0488 98 26 5.500 3.46E+4 5.19E+3 C0488 98 27 6.000 6.85E+4 1.03E+4 C0488 98 28 6.500 1.22E+5 1.83E+4 C0488 98 29 7.000 2.01E+5 3.02E+4 C0488 98 30 7.500 3.09E+5 5.50E+4 C0488 98 31 8.000 4.49E+5 9.46E+4 C0488 98 32 ENDDATA 14 0 C0488 98 33 ENDSUBENT 32 0 C0488 9899999 SUBENT C0488099 20160324 C158C0488 99 1 BIB 5 13 C0488 99 2 REACTION (52-TE-126(P,N)53-I-126,,SGV) C0488 99 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488 99 4 directly from measured reaction cross sections and C0488 99 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488 99 7 value of the product of the cross section times the C0488 99 8 velocity, averaged over the Maxwell-Boltzmann C0488 99 9 velocity distribution at the temperature T of interest.C0488 99 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488 99 11 their values were added quadratically. C0488 99 12 STATUS (TABLE) Table III, page 193. C0488 99 13 (DEP,C0488027) C0488 99 14 HISTORY (20160324C) BP C0488 99 15 ENDBIB 13 0 C0488 99 16 NOCOMMON 0 0 C0488 99 17 DATA 3 12 C0488 99 18 KT DATA DATA-ERR C0488 99 19 K9 CM3/S/MOL CM3/S/MOL C0488 99 20 2.500 2.01E+0 3.02E-1 C0488 99 21 3.000 2.49E+1 3.73E+0 C0488 99 22 3.500 1.68E+2 2.52E+1 C0488 99 23 4.000 7.55E+2 1.13E+2 C0488 99 24 4.500 2.54E+3 3.81E+2 C0488 99 25 5.000 6.91E+3 1.04E+3 C0488 99 26 5.500 1.59E+4 2.39E+3 C0488 99 27 6.000 3.21E+4 4.82E+3 C0488 99 28 6.500 5.84E+4 9.75E+3 C0488 99 29 7.000 9.77E+4 2.04E+4 C0488 99 30 7.500 1.53E+5 3.87E+4 C0488 99 31 8.000 2.25E+5 6.73E+4 C0488 99 32 ENDDATA 14 0 C0488 99 33 ENDSUBENT 32 0 C0488 9999999 SUBENT C0488100 20160324 C158C0488100 1 BIB 5 13 C0488100 2 REACTION (52-TE-128(P,N)53-I-128,,SGV) C0488100 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488100 4 directly from measured reaction cross sections and C0488100 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488100 7 value of the product of the cross section times the C0488100 8 velocity, averaged over the Maxwell-Boltzmann C0488100 9 velocity distribution at the temperature T of interest.C0488100 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488100 11 their values were added quadratically. C0488100 12 STATUS (TABLE) Table III, page 193. C0488100 13 (DEP,C0488028) C0488100 14 HISTORY (20160324C) BP C0488100 15 ENDBIB 13 0 C0488100 16 NOCOMMON 0 0 C0488100 17 DATA 3 12 C0488100 18 KT DATA DATA-ERR C0488100 19 K9 CM3/S/MOL CM3/S/MOL C0488100 20 2.500 1.73E+0 2.59E-1 C0488100 21 3.000 1.85E+1 2.78E+0 C0488100 22 3.500 1.14E+2 1.71E+1 C0488100 23 4.000 4.85E+2 7.28E+1 C0488100 24 4.500 1.59E+3 2.39E+2 C0488100 25 5.000 4.28E+3 6.42E+2 C0488100 26 5.500 9.83E+3 1.47E+3 C0488100 27 6.000 1.99E+4 3.44E+3 C0488100 28 6.500 3.66E+4 8.31E+3 C0488100 29 7.000 6.18E+4 1.76E+4 C0488100 30 7.500 9.75E+4 3.35E+4 C0488100 31 8.000 1.45E+5 5.89E+4 C0488100 32 ENDDATA 14 0 C0488100 33 ENDSUBENT 32 0 C048810099999 SUBENT C0488101 20160324 C158C0488101 1 BIB 5 13 C0488101 2 REACTION (52-TE-130(P,N)53-I-130,,SGV) C0488101 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488101 4 directly from measured reaction cross sections and C0488101 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488101 7 value of the product of the cross section times the C0488101 8 velocity, averaged over the Maxwell-Boltzmann C0488101 9 velocity distribution at the temperature T of interest.C0488101 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488101 11 their values were added quadratically. C0488101 12 STATUS (TABLE) Table III, page 193. C0488101 13 (DEP,C0488029) C0488101 14 HISTORY (20160324C) BP C0488101 15 ENDBIB 13 0 C0488101 16 NOCOMMON 0 0 C0488101 17 DATA 3 12 C0488101 18 KT DATA DATA-ERR C0488101 19 K9 CM3/S/MOL CM3/S/MOL C0488101 20 2.500 2.86E+0 9.67E-1 C0488101 21 3.000 2.72E+1 4.27E+0 C0488101 22 3.500 1.60E+2 2.40E+1 C0488101 23 4.000 6.79E+2 1.02E+2 C0488101 24 4.500 2.24E+3 3.36E+2 C0488101 25 5.000 6.04E+3 9.06E+2 C0488101 26 5.500 1.40E+4 2.10E+3 C0488101 27 6.000 2.84E+4 4.69E+3 C0488101 28 6.500 5.22E+4 1.12E+4 C0488101 29 7.000 8.83E+4 2.36E+4 C0488101 30 7.500 1.39E+5 4.49E+4 C0488101 31 8.000 2.08E+5 7.90E+4 C0488101 32 ENDDATA 14 0 C0488101 33 ENDSUBENT 32 0 C048810199999 SUBENT C0488102 20160324 C158C0488102 1 BIB 5 13 C0488102 2 REACTION (52-TE-130(P,N)53-I-130-M,,SGV) C0488102 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488102 4 directly from measured reaction cross sections and C0488102 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488102 7 value of the product of the cross section times the C0488102 8 velocity, averaged over the Maxwell-Boltzmann C0488102 9 velocity distribution at the temperature T of interest.C0488102 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488102 11 their values were added quadratically. C0488102 12 STATUS (TABLE) Table III, page 193. C0488102 13 (DEP,C0488030) C0488102 14 HISTORY (20160324C) BP C0488102 15 ENDBIB 13 0 C0488102 16 NOCOMMON 0 0 C0488102 17 DATA 3 12 C0488102 18 KT DATA DATA-ERR C0488102 19 K9 CM3/S/MOL CM3/S/MOL C0488102 20 2.500 6.81E+0 3.34E+0 C0488102 21 3.000 5.09E+1 1.48E+1 C0488102 22 3.500 2.31E+2 4.07E+1 C0488102 23 4.000 7.69E+2 1.15E+2 C0488102 24 4.500 2.08E+3 3.12E+2 C0488102 25 5.000 4.83E+3 7.25E+2 C0488102 26 5.500 9.97E+3 1.50E+3 C0488102 27 6.000 1.87E+4 2.81E+3 C0488102 28 6.500 3.23E+4 5.72E+3 C0488102 29 7.000 5.21E+4 1.20E+4 C0488102 30 7.500 7.95E+4 2.30E+4 C0488102 31 8.000 1.16E+5 4.05E+4 C0488102 32 ENDDATA 14 0 C0488102 33 ENDSUBENT 32 0 C048810299999 SUBENT C0488103 20160324 C158C0488103 1 BIB 5 13 C0488103 2 REACTION (56-BA-134(P,N)57-LA-134,,SGV) C0488103 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488103 4 directly from measured reaction cross sections and C0488103 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488103 7 value of the product of the cross section times the C0488103 8 velocity, averaged over the Maxwell-Boltzmann C0488103 9 velocity distribution at the temperature T of interest.C0488103 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488103 11 their values were added quadratically. C0488103 12 STATUS (TABLE) Table III, page 193. C0488103 13 (DEP,C0488031) C0488103 14 HISTORY (20160324C) BP C0488103 15 ENDBIB 13 0 C0488103 16 NOCOMMON 0 0 C0488103 17 DATA 3 10 C0488103 18 KT DATA DATA-ERR C0488103 19 K9 CM3/S/MOL CM3/S/MOL C0488103 20 2.500 2.09E-2 3.14E-3 C0488103 21 3.000 7.31E-1 1.10E-1 C0488103 22 3.500 9.44E+0 1.42E+0 C0488103 23 4.000 6.50E+1 9.75E+0 C0488103 24 4.500 2.93E+2 4.40E+1 C0488103 25 5.000 9.76E+2 1.92E+2 C0488103 26 5.500 2.61E+3 6.73E+2 C0488103 27 6.000 5.92E+3 1.91E+3 C0488103 28 6.500 1.18E+4 4.61E+3 C0488103 29 7.000 2.11E+4 9.75E+3 C0488103 30 ENDDATA 12 0 C0488103 31 ENDSUBENT 30 0 C048810399999 SUBENT C0488104 20160324 C158C0488104 1 BIB 5 13 C0488104 2 REACTION (56-BA-136(P,N)57-LA-136,,SGV) C0488104 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488104 4 directly from measured reaction cross sections and C0488104 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488104 7 value of the product of the cross section times the C0488104 8 velocity, averaged over the Maxwell-Boltzmann C0488104 9 velocity distribution at the temperature T of interest.C0488104 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488104 11 their values were added quadratically. C0488104 12 STATUS (TABLE) Table III, page 193. C0488104 13 (DEP,C0488032) C0488104 14 HISTORY (20160324C) BP C0488104 15 ENDBIB 13 0 C0488104 16 NOCOMMON 0 0 C0488104 17 DATA 3 12 C0488104 18 KT DATA DATA-ERR C0488104 19 K9 CM3/S/MOL CM3/S/MOL C0488104 20 2.500 2.00E-1 3.00E-2 C0488104 21 3.000 3.63E+0 5.44E-1 C0488104 22 3.500 3.06E+1 4.59E+0 C0488104 23 4.000 1.59E+2 2.39E+1 C0488104 24 4.500 5.95E+2 8.93E+1 C0488104 25 5.000 1.74E+3 2.61E+2 C0488104 26 5.500 4.26E+3 6.73E+2 C0488104 27 6.000 9.04E+3 1.89E+3 C0488104 28 6.500 1.71E+4 4.53E+3 C0488104 29 7.000 2.96E+4 9.59E+3 C0488104 30 7.500 4.75E+4 1.82E+4 C0488104 31 8.000 7.19E+4 3.21E+4 C0488104 32 ENDDATA 14 0 C0488104 33 ENDSUBENT 32 0 C048810499999 SUBENT C0488105 20160324 C158C0488105 1 BIB 5 13 C0488105 2 REACTION (60-ND-143(P,N)61-PM-143,,SGV) C0488105 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488105 4 directly from measured reaction cross sections and C0488105 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488105 7 value of the product of the cross section times the C0488105 8 velocity, averaged over the Maxwell-Boltzmann C0488105 9 velocity distribution at the temperature T of interest.C0488105 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488105 11 their values were added quadratically. C0488105 12 STATUS (TABLE) Table III, page 193. C0488105 13 (DEP,C0488033) C0488105 14 HISTORY (20160324C) BP C0488105 15 ENDBIB 13 0 C0488105 16 NOCOMMON 0 0 C0488105 17 DATA 3 8 C0488105 18 KT DATA DATA-ERR C0488105 19 K9 CM3/S/MOL CM3/S/MOL C0488105 20 3.500 1.67E+1 7.87E+0 C0488105 21 4.000 1.02E+2 3.85E+1 C0488105 22 4.500 4.17E+2 1.42E+2 C0488105 23 5.000 1.28E+3 4.44E+2 C0488105 24 5.500 3.21E+3 1.22E+3 C0488105 25 6.000 6.86E+3 2.94E+3 C0488105 26 6.500 1.30E+4 6.36E+3 C0488105 27 7.000 2.23E+4 1.24E+4 C0488105 28 ENDDATA 10 0 C0488105 29 ENDSUBENT 28 0 C048810599999 SUBENT C0488106 20160324 C158C0488106 1 BIB 5 13 C0488106 2 REACTION (60-ND-144(P,N)61-PM-144,,SGV) C0488106 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488106 4 directly from measured reaction cross sections and C0488106 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488106 7 value of the product of the cross section times the C0488106 8 velocity, averaged over the Maxwell-Boltzmann C0488106 9 velocity distribution at the temperature T of interest.C0488106 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488106 11 their values were added quadratically. C0488106 12 STATUS (TABLE) Table III, page 193. C0488106 13 (DEP,C0488034) C0488106 14 HISTORY (20160324C) BP C0488106 15 ENDBIB 13 0 C0488106 16 NOCOMMON 0 0 C0488106 17 DATA 3 8 C0488106 18 KT DATA DATA-ERR C0488106 19 K9 CM3/S/MOL CM3/S/MOL C0488106 20 2.500 1.07E-1 4.44E-2 C0488106 21 3.000 1.81E+0 5.26E-1 C0488106 22 3.500 1.46E+1 2.72E+0 C0488106 23 4.000 7.48E+1 1.12E+1 C0488106 24 4.500 2.78E+2 6.20E+1 C0488106 25 5.000 8.15E+2 2.48E+2 C0488106 26 5.500 2.00E+3 7.99E+2 C0488106 27 6.000 4.24E+3 2.13E+3 C0488106 28 ENDDATA 10 0 C0488106 29 ENDSUBENT 28 0 C048810699999 SUBENT C0488107 20160324 C158C0488107 1 BIB 5 13 C0488107 2 REACTION (60-ND-146(P,N)61-PM-146,,SGV) C0488107 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488107 4 directly from measured reaction cross sections and C0488107 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488107 7 value of the product of the cross section times the C0488107 8 velocity, averaged over the Maxwell-Boltzmann C0488107 9 velocity distribution at the temperature T of interest.C0488107 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488107 11 their values were added quadratically. C0488107 12 STATUS (TABLE) Table III, page 193. C0488107 13 (DEP,C0488035) C0488107 14 HISTORY (20160324C) BP C0488107 15 ENDBIB 13 0 C0488107 16 NOCOMMON 0 0 C0488107 17 DATA 3 8 C0488107 18 KT DATA DATA-ERR C0488107 19 K9 CM3/S/MOL CM3/S/MOL C0488107 20 3.500 4.54E+1 6.81E+0 C0488107 21 4.000 2.10E+2 6.47E+1 C0488107 22 4.500 7.14E+2 1.79E+2 C0488107 23 5.000 1.95E+3 4.82E+2 C0488107 24 5.500 4.48E+3 1.26E+3 C0488107 25 6.000 9.04E+3 3.07E+3 C0488107 26 6.500 1.65E+4 6.76E+3 C0488107 27 7.000 2.75E+4 1.34E+4 C0488107 28 ENDDATA 10 0 C0488107 29 ENDSUBENT 28 0 C048810799999 SUBENT C0488108 20160324 C158C0488108 1 BIB 5 13 C0488108 2 REACTION (60-ND-148(P,N)61-PM-148,,SGV) C0488108 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488108 4 directly from measured reaction cross sections and C0488108 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488108 7 value of the product of the cross section times the C0488108 8 velocity, averaged over the Maxwell-Boltzmann C0488108 9 velocity distribution at the temperature T of interest.C0488108 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488108 11 their values were added quadratically. C0488108 12 STATUS (TABLE) Table III, page 194. C0488108 13 (DEP,C0488036) C0488108 14 HISTORY (20160324C) BP C0488108 15 ENDBIB 13 0 C0488108 16 NOCOMMON 0 0 C0488108 17 DATA 3 9 C0488108 18 KT DATA DATA-ERR C0488108 19 K9 CM3/S/MOL CM3/S/MOL C0488108 20 3.000 1.23E+0 7.12E-1 C0488108 21 3.500 9.84E+0 3.39E+0 C0488108 22 4.000 4.99E+1 1.23E+1 C0488108 23 4.500 1.83E+2 4.24E+1 C0488108 24 5.000 5.31E+2 1.44E+2 C0488108 25 5.500 1.25E+3 4.33E+2 C0488108 26 6.000 2.69E+3 1.12E+3 C0488108 27 6.500 5.05E+3 2.53E+3 C0488108 28 7.000 8.64E+3 5.45E+3 C0488108 29 ENDDATA 11 0 C0488108 30 ENDSUBENT 29 0 C048810899999 SUBENT C0488109 20160324 C158C0488109 1 BIB 5 13 C0488109 2 REACTION (60-ND-148(P,N)61-PM-148-M,,SGV) C0488109 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488109 4 directly from measured reaction cross sections and C0488109 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488109 7 value of the product of the cross section times the C0488109 8 velocity, averaged over the Maxwell-Boltzmann C0488109 9 velocity distribution at the temperature T of interest.C0488109 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488109 11 their values were added quadratically. C0488109 12 STATUS (TABLE) Table III, page 194. C0488109 13 (DEP,C0488037) C0488109 14 HISTORY (20160324C) BP C0488109 15 ENDBIB 13 0 C0488109 16 NOCOMMON 0 0 C0488109 17 DATA 3 7 C0488109 18 KT DATA DATA-ERR C0488109 19 K9 CM3/S/MOL CM3/S/MOL C0488109 20 5.000 1.44E+3 1.13E+3 C0488109 21 5.500 3.42E+3 2.48E+3 C0488109 22 6.000 7.02E+3 4.93E+3 C0488109 23 6.500 1.29E+4 9.18E+3 C0488109 24 7.000 2.16E+4 1.60E+4 C0488109 25 7.500 3.36E+4 2.66E+4 C0488109 26 8.000 4.95E+4 4.22E+4 C0488109 27 ENDDATA 9 0 C0488109 28 ENDSUBENT 27 0 C048810999999 SUBENT C0488110 20160324 C158C0488110 1 BIB 5 13 C0488110 2 REACTION (60-ND-150(P,N)61-PM-150,,SGV) C0488110 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488110 4 directly from measured reaction cross sections and C0488110 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488110 7 value of the product of the cross section times the C0488110 8 velocity, averaged over the Maxwell-Boltzmann C0488110 9 velocity distribution at the temperature T of interest.C0488110 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488110 11 their values were added quadratically. C0488110 12 STATUS (TABLE) Table III, page 194. C0488110 13 (DEP,C0488038) C0488110 14 HISTORY (20160324C) BP C0488110 15 ENDBIB 13 0 C0488110 16 NOCOMMON 0 0 C0488110 17 DATA 3 10 C0488110 18 KT DATA DATA-ERR C0488110 19 K9 CM3/S/MOL CM3/S/MOL C0488110 20 1.500 4.83E-4 1.08E-4 C0488110 21 2.000 2.22E-1 3.33E-2 C0488110 22 2.500 1.14E+1 1.71E+0 C0488110 23 3.000 1.85E+2 2.78E+1 C0488110 24 3.500 1.51E+3 2.27E+2 C0488110 25 4.000 7.78E+3 1.17E+3 C0488110 26 4.500 2.91E+4 5.38E+3 C0488110 27 5.000 8.56E+4 2.30E+4 C0488110 28 5.500 2.10E+5 7.60E+4 C0488110 29 6.000 4.44E+5 2.04E+5 C0488110 30 ENDDATA 12 0 C0488110 31 ENDSUBENT 30 0 C048811099999 SUBENT C0488111 20160324 C158C0488111 1 BIB 5 13 C0488111 2 REACTION (62-SM-147(P,N)63-EU-147,,SGV) C0488111 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488111 4 directly from measured reaction cross sections and C0488111 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488111 7 value of the product of the cross section times the C0488111 8 velocity, averaged over the Maxwell-Boltzmann C0488111 9 velocity distribution at the temperature T of interest.C0488111 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488111 11 their values were added quadratically. C0488111 12 STATUS (TABLE) Table III, page 194. C0488111 13 (DEP,C0488039) C0488111 14 HISTORY (20160324C) BP C0488111 15 ENDBIB 13 0 C0488111 16 NOCOMMON 0 0 C0488111 17 DATA 3 12 C0488111 18 KT DATA DATA-ERR C0488111 19 K9 CM3/S/MOL CM3/S/MOL C0488111 20 2.500 5.41E-1 1.90E-1 C0488111 21 3.000 5.31E+0 1.09E+0 C0488111 22 3.500 3.17E+1 4.76E+0 C0488111 23 4.000 1.38E+2 2.07E+1 C0488111 24 4.500 4.75E+2 7.13E+1 C0488111 25 5.000 1.34E+3 2.01E+2 C0488111 26 5.500 3.22E+3 4.83E+2 C0488111 27 6.000 6.78E+3 1.02E+3 C0488111 28 6.500 1.28E+4 1.92E+3 C0488111 29 7.000 2.20E+4 3.30E+3 C0488111 30 7.500 3.53E+4 5.30E+3 C0488111 31 8.000 5.31E+4 7.97E+3 C0488111 32 ENDDATA 14 0 C0488111 33 ENDSUBENT 32 0 C048811199999 SUBENT C0488112 20160324 C158C0488112 1 BIB 5 13 C0488112 2 REACTION (62-SM-148(P,N)63-EU-148,,SGV) C0488112 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488112 4 directly from measured reaction cross sections and C0488112 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488112 7 value of the product of the cross section times the C0488112 8 velocity, averaged over the Maxwell-Boltzmann C0488112 9 velocity distribution at the temperature T of interest.C0488112 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488112 11 their values were added quadratically. C0488112 12 STATUS (TABLE) Table III, page 194. C0488112 13 (DEP,C0488040) C0488112 14 HISTORY (20160324C) BP C0488112 15 ENDBIB 13 0 C0488112 16 NOCOMMON 0 0 C0488112 17 DATA 3 11 C0488112 18 KT DATA DATA-ERR C0488112 19 K9 CM3/S/MOL CM3/S/MOL C0488112 20 2.500 3.76E-2 5.64E-3 C0488112 21 3.000 8.22E-1 1.23E-1 C0488112 22 3.500 8.23E+0 1.23E+0 C0488112 23 4.000 5.01E+1 7.52E+0 C0488112 24 4.500 2.16E+2 3.24E+1 C0488112 25 5.000 7.17E+2 1.08E+2 C0488112 26 5.500 1.95E+3 3.67E+2 C0488112 27 6.000 4.55E+3 1.14E+3 C0488112 28 6.500 9.35E+3 2.97E+3 C0488112 29 7.000 1.74E+4 6.75E+3 C0488112 30 7.500 2.97E+4 1.37E+4 C0488112 31 ENDDATA 13 0 C0488112 32 ENDSUBENT 31 0 C048811299999 SUBENT C0488113 20160324 C158C0488113 1 BIB 5 13 C0488113 2 REACTION (62-SM-149(P,N)63-EU-149,,SGV) C0488113 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488113 4 directly from measured reaction cross sections and C0488113 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488113 7 value of the product of the cross section times the C0488113 8 velocity, averaged over the Maxwell-Boltzmann C0488113 9 velocity distribution at the temperature T of interest.C0488113 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488113 11 their values were added quadratically. C0488113 12 STATUS (TABLE) Table III, page 194. C0488113 13 (DEP,C0488041) C0488113 14 HISTORY (20160324C) BP C0488113 15 ENDBIB 13 0 C0488113 16 NOCOMMON 0 0 C0488113 17 DATA 3 7 C0488113 18 KT DATA DATA-ERR C0488113 19 K9 CM3/S/MOL CM3/S/MOL C0488113 20 5.000 4.13E+3 2.72E+3 C0488113 21 5.500 6.95E+3 3.78E+3 C0488113 22 6.000 1.08E+4 5.27E+3 C0488113 23 6.500 1.61E+4 6.10E+3 C0488113 24 7.000 2.28E+4 7.41E+3 C0488113 25 7.500 3.14E+4 9.14E+3 C0488113 26 8.000 4.20E+4 1.17E+4 C0488113 27 ENDDATA 9 0 C0488113 28 ENDSUBENT 27 0 C048811399999 SUBENT C0488114 20160324 C158C0488114 1 BIB 5 13 C0488114 2 REACTION (62-SM-150(P,N)63-EU-150,,SGV) C0488114 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488114 4 directly from measured reaction cross sections and C0488114 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488114 7 value of the product of the cross section times the C0488114 8 velocity, averaged over the Maxwell-Boltzmann C0488114 9 velocity distribution at the temperature T of interest.C0488114 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488114 11 their values were added quadratically. C0488114 12 STATUS (TABLE) Table III, page 194. C0488114 13 (DEP,C0488042) C0488114 14 HISTORY (20160324C) BP C0488114 15 ENDBIB 13 0 C0488114 16 NOCOMMON 0 0 C0488114 17 DATA 3 12 C0488114 18 KT DATA DATA-ERR C0488114 19 K9 CM3/S/MOL CM3/S/MOL C0488114 20 2.500 1.90E-1 2.85E-2 C0488114 21 3.000 2.21E+0 3.32E-1 C0488114 22 3.500 1.40E+1 2.10E+0 C0488114 23 4.000 6.25E+1 9.38E+0 C0488114 24 4.500 2.18E+2 3.27E+1 C0488114 25 5.000 6.31E+2 9.47E+1 C0488114 26 5.500 1.57E+3 2.36E+2 C0488114 27 6.000 3.46E+3 7.27E+2 C0488114 28 6.500 6.83E+3 1.90E+3 C0488114 29 7.000 1.24E+4 4.33E+3 C0488114 30 7.500 2.07E+4 8.76E+3 C0488114 31 8.000 3.27E+4 1.63E+4 C0488114 32 ENDDATA 14 0 C0488114 33 ENDSUBENT 32 0 C048811499999 SUBENT C0488115 20160324 C158C0488115 1 BIB 5 13 C0488115 2 REACTION (62-SM-152(P,N)63-EU-152,,SGV) C0488115 3 ANALYSIS Thermonuclear reaction rates are usually calculated C0488115 4 directly from measured reaction cross sections and C0488115 5 level parameters. The relevant quantity is NA T which is Avogadro's number times the average C0488115 7 value of the product of the cross section times the C0488115 8 velocity, averaged over the Maxwell-Boltzmann C0488115 9 velocity distribution at the temperature T of interest.C0488115 10 ERR-ANALYS (DATA-ERR) List of uncertainties is incomplete, C0488115 11 their values were added quadratically. C0488115 12 STATUS (TABLE) Table III, page 194. C0488115 13 (DEP,C0488043) C0488115 14 HISTORY (20160324C) BP C0488115 15 ENDBIB 13 0 C0488115 16 NOCOMMON 0 0 C0488115 17 DATA 3 13 C0488115 18 KT DATA DATA-ERR C0488115 19 K9 CM3/S/MOL CM3/S/MOL C0488115 20 2.000 7.21E-3 2.29E-3 C0488115 21 2.500 2.11E-1 3.80E-2 C0488115 22 3.000 2.32E+0 3.48E-1 C0488115 23 3.500 1.52E+1 2.28E+0 C0488115 24 4.000 7.08E+1 1.06E+1 C0488115 25 4.500 2.57E+2 3.86E+1 C0488115 26 5.000 7.65E+2 1.15E+2 C0488115 27 5.500 1.93E+3 2.90E+2 C0488115 28 6.000 4.26E+3 7.37E+2 C0488115 29 6.500 8.40E+3 1.91E+3 C0488115 30 7.000 1.51E+4 4.29E+3 C0488115 31 7.500 2.52E+4 8.64E+3 C0488115 32 8.000 3.95E+4 1.60E+4 C0488115 33 ENDDATA 15 0 C0488115 34 ENDSUBENT 33 0 C048811599999 ENDENTRY 115 0 C048899999999