ENTRY C1584 20160318 C158C158400000001 SUBENT C1584001 20160318 C158C158400100001 BIB 8 13 C158400100002 TITLE Thick-target measurements and astrophysical C158400100003 thermonuclear reaction rates: Alpha-induced reactions C158400100004 AUTHOR (N.A.Roughton,T.P.Intrator,R.J.Peterson,C.S.Zaidins, C158400100005 C.J.Hansen) C158400100006 REFERENCE (J,AND,28,(2),341,1983) C158400100007 #doi:10.1016/0092-640X(83)90021-9 C158400100008 REL-REF (M,C0488001,N.A.Roughton+,J,AND,23,(2),177,1979) C158400100009 INSTITUTE (1USACLU,1USANBS) C158400100010 FACILITY (CYCLO,1USACLU) University of Colorado Variable C158400100011 Energy Cyclotron facility. C158400100012 DETECTOR (GELI) Detector calibration results: energy is within C158400100013 3 keV and efficiency is within 5%. C158400100014 HISTORY (20160318C) BP C158400100015 ENDBIB 13 0 C158400100016 NOCOMMON 0 0 C158400100017 ENDSUBENT 16 0 C158400199999 SUBENT C1584002 20160318 C158C158400200001 BIB 5 15 C158400200002 REACTION (5-B-10(A,N)7-N-13,,PY,,TT) C158400200003 METHOD (ACTIV) C158400200004 PART-DET (DG) C158400200005 ERR-ANALYS (DATA-ERR) The uncertainty in the yields is either C158400200006 statistical, due to the number of gamma-ray counts, C158400200007 or set to 7% due to uncertainties in the beam C158400200008 integration, target location, and detector efficiency, C158400200009 whichever is larger. This 7% figure is due to an C158400200010 uncertainty of approximately 5% in bombardment C158400200011 parameters such as current integration and 5% in C158400200012 counting due to source location, and so forth. These C158400200013 uncertainties are then added quadratically. C158400200014 (ERR-1) Bombardment parameters. C158400200015 (ERR-2) Source location. C158400200016 STATUS (TABLE) Table II, page 346. C158400200017 ENDBIB 15 0 C158400200018 COMMON 2 3 C158400200019 ERR-1 ERR-2 C158400200020 PER-CENT PER-CENT C158400200021 5.0 5.0 C158400200022 ENDCOMMON 3 0 C158400200023 DATA 3 21 C158400200024 EN DATA DATA-ERR C158400200025 MEV PRD/INC PRD/INC C158400200026 3.214 3.8E-7 4.0E-8 C158400200027 3.370 2.8E-7 5.0E-8 C158400200028 3.988 6.1E-7 6.0E-8 C158400200029 4.050 6.7E-7 6.0E-8 C158400200030 4.389 9.5E-7 9.0E-8 C158400200031 4.896 1.4E-6 2.0E-7 C158400200032 5.261 1.7E-6 3.0E-7 C158400200033 5.436 1.5E-6 3.0E-7 C158400200034 6.204 2.2E-6 3.0E-7 C158400200035 6.965 3.4E-6 4.0E-7 C158400200036 7.205 3.8E-6 5.0E-7 C158400200037 7.251 2.7E-6 1.0E-6 C158400200038 7.596 4.4E-6 8.0E-7 C158400200039 9.160 6.6E-6 1.0E-6 C158400200040 9.210 7.3E-6 1.0E-6 C158400200041 9.899 8.1E-6 1.0E-6 C158400200042 9.973 6.7E-6 1.0E-6 C158400200043 10.682 9.8E-6 1.0E-6 C158400200044 11.250 1.1E-5 1.0E-6 C158400200045 12.370 9.2E-6 1.0E-6 C158400200046 14.169 1.1E-5 1.0E-6 C158400200047 ENDDATA 23 0 C158400200048 ENDSUBENT 47 0 C158400299999 SUBENT C1584003 20160318 C158C158400300001 BIB 5 15 C158400300002 REACTION (7-N-14(A,N)9-F-17,,PY,,TT) C158400300003 METHOD (ACTIV) C158400300004 PART-DET (DG) C158400300005 ERR-ANALYS (DATA-ERR) The uncertainty in the yields is either C158400300006 statistical, due to the number of gamma-ray counts, C158400300007 or set to 7% due to uncertainties in the beam C158400300008 integration, target location, and detector efficiency, C158400300009 whichever is larger. This 7% figure is due to an C158400300010 uncertainty of approximately 5% in bombardment C158400300011 parameters such as current integration and 5% in C158400300012 counting due to source location, and so forth. These C158400300013 uncertainties are then added quadratically. C158400300014 (ERR-1) Bombardment parameters. C158400300015 (ERR-2) Source location. C158400300016 STATUS (TABLE) Table II, page 346. C158400300017 ENDBIB 15 0 C158400300018 COMMON 2 3 C158400300019 ERR-1 ERR-2 C158400300020 PER-CENT PER-CENT C158400300021 5.0 5.0 C158400300022 ENDCOMMON 3 0 C158400300023 DATA 3 8 C158400300024 EN DATA DATA-ERR C158400300025 MEV PRD/INC PRD/INC C158400300026 6.219 3.6E-7 1.0E-7 C158400300027 6.965 1.4E-6 2.0E-7 C158400300028 7.265 2.3E-6 5.0E-7 C158400300029 8.421 1.6E-5 2.0E-6 C158400300030 9.899 1.9E-5 2.0E-6 C158400300031 10.682 2.7E-5 3.0E-6 C158400300032 11.277 3.1E-5 3.0E-6 C158400300033 16.799 4.1E-5 4.0E-6 C158400300034 ENDDATA 10 0 C158400300035 ENDSUBENT 34 0 C158400399999 SUBENT C1584004 20160318 C158C158400400001 BIB 5 15 C158400400002 REACTION (7-N-14(A,G)9-F-18,,PY,,TT) C158400400003 METHOD (ACTIV) C158400400004 PART-DET (DG) C158400400005 ERR-ANALYS (DATA-ERR) The uncertainty in the yields is either C158400400006 statistical, due to the number of gamma-ray counts, C158400400007 or set to 7% due to uncertainties in the beam C158400400008 integration, target location, and detector efficiency, C158400400009 whichever is larger. This 7% figure is due to an C158400400010 uncertainty of approximately 5% in bombardment C158400400011 parameters such as current integration and 5% in C158400400012 counting due to source location, and so forth. These C158400400013 uncertainties are then added quadratically. C158400400014 (ERR-1) Bombardment parameters. C158400400015 (ERR-2) Source location. C158400400016 STATUS (TABLE) Table II, page 346. C158400400017 ENDBIB 15 0 C158400400018 COMMON 2 3 C158400400019 ERR-1 ERR-2 C158400400020 PER-CENT PER-CENT C158400400021 5.0 5.0 C158400400022 ENDCOMMON 3 0 C158400400023 DATA 3 2 C158400400024 EN DATA DATA-ERR C158400400025 MEV PRD/INC PRD/INC C158400400026 6.219 1.6E-9 4.0E-10 C158400400027 7.265 7.0E-9 2.0E-9 C158400400028 ENDDATA 4 0 C158400400029 ENDSUBENT 28 0 C158400499999 SUBENT C1584005 20160318 C158C158400500001 BIB 5 15 C158400500002 REACTION (7-N-15(A,N)9-F-18,,PY,,TT) C158400500003 METHOD (ACTIV) C158400500004 PART-DET (DG) C158400500005 ERR-ANALYS (DATA-ERR) The uncertainty in the yields is either C158400500006 statistical, due to the number of gamma-ray counts, C158400500007 or set to 7% due to uncertainties in the beam C158400500008 integration, target location, and detector efficiency, C158400500009 whichever is larger. This 7% figure is due to an C158400500010 uncertainty of approximately 5% in bombardment C158400500011 parameters such as current integration and 5% in C158400500012 counting due to source location, and so forth. These C158400500013 uncertainties are then added quadratically. C158400500014 (ERR-1) Bombardment parameters. C158400500015 (ERR-2) Source location. C158400500016 STATUS (TABLE) Table II, page 346. C158400500017 ENDBIB 15 0 C158400500018 COMMON 2 3 C158400500019 ERR-1 ERR-2 C158400500020 PER-CENT PER-CENT C158400500021 5.0 5.0 C158400500022 ENDCOMMON 3 0 C158400500023 DATA 3 4 C158400500024 EN DATA DATA-ERR C158400500025 MEV PRD/INC PRD/INC C158400500026 8.421 1.2E-7 3.0E-8 C158400500027 10.682 4.0E-7 4.0E-8 C158400500028 11.277 5.8E-7 7.0E-8 C158400500029 16.799 3.1E-6 4.0E-7 C158400500030 ENDDATA 6 0 C158400500031 ENDSUBENT 30 0 C158400599999 SUBENT C1584006 20160318 C158C158400600001 BIB 5 15 C158400600002 REACTION (12-MG-25(A,P)13-AL-28,,PY,,TT) C158400600003 METHOD (ACTIV) C158400600004 PART-DET (DG) C158400600005 ERR-ANALYS (DATA-ERR) The uncertainty in the yields is either C158400600006 statistical, due to the number of gamma-ray counts, C158400600007 or set to 7% due to uncertainties in the beam C158400600008 integration, target location, and detector efficiency, C158400600009 whichever is larger. This 7% figure is due to an C158400600010 uncertainty of approximately 5% in bombardment C158400600011 parameters such as current integration and 5% in C158400600012 counting due to source location, and so forth. These C158400600013 uncertainties are then added quadratically. C158400600014 (ERR-1) Bombardment parameters. C158400600015 (ERR-2) Source location. C158400600016 STATUS (TABLE) Table II, page 346. C158400600017 ENDBIB 15 0 C158400600018 COMMON 2 3 C158400600019 ERR-1 ERR-2 C158400600020 PER-CENT PER-CENT C158400600021 5.0 5.0 C158400600022 ENDCOMMON 3 0 C158400600023 DATA 3 11 C158400600024 EN DATA DATA-ERR C158400600025 MEV PRD/INC PRD/INC C158400600026 3.442 1.1E-8 2.0E-9 C158400600027 3.643 2.0E-8 2.0E-9 C158400600028 3.924 4.1E-8 2.0E-9 C158400600029 4.549 3.3E-7 2.0E-8 C158400600030 5.080 8.2E-7 6.0E-8 C158400600031 5.395 1.5E-6 1.0E-7 C158400600032 5.785 2.5E-6 2.0E-7 C158400600033 6.226 4.3E-6 3.0E-7 C158400600034 6.250 4.5E-6 3.0E-7 C158400600035 9.749 3.8E-5 3.0E-6 C158400600036 13.074 4.7E-5 4.0E-6 C158400600037 ENDDATA 13 0 C158400600038 ENDSUBENT 37 0 C158400699999 SUBENT C1584007 20160318 C158C158400700001 BIB 5 15 C158400700002 REACTION (12-MG-26(A,P)13-AL-29,,PY,,TT) C158400700003 METHOD (ACTIV) C158400700004 PART-DET (DG) C158400700005 ERR-ANALYS (DATA-ERR) The uncertainty in the yields is either C158400700006 statistical, due to the number of gamma-ray counts, C158400700007 or set to 7% due to uncertainties in the beam C158400700008 integration, target location, and detector efficiency, C158400700009 whichever is larger. This 7% figure is due to an C158400700010 uncertainty of approximately 5% in bombardment C158400700011 parameters such as current integration and 5% in C158400700012 counting due to source location, and so forth. These C158400700013 uncertainties are then added quadratically. C158400700014 (ERR-1) Bombardment parameters. C158400700015 (ERR-2) Source location. C158400700016 STATUS (TABLE) Table II, page 346. C158400700017 ENDBIB 15 0 C158400700018 COMMON 2 3 C158400700019 ERR-1 ERR-2 C158400700020 PER-CENT PER-CENT C158400700021 5.0 5.0 C158400700022 ENDCOMMON 3 0 C158400700023 DATA 3 9 C158400700024 EN DATA DATA-ERR C158400700025 MEV PRD/INC PRD/INC C158400700026 3.924 4.0E-10 3.0E-10 C158400700027 4.549 7.0E-9 2.0E-9 C158400700028 5.080 3.0E-8 3.0E-9 C158400700029 5.395 1.2E-7 1.0E-8 C158400700030 5.785 3.1E-7 3.0E-8 C158400700031 6.226 4.4E-7 4.0E-8 C158400700032 6.250 4.9E-7 5.0E-8 C158400700033 9.749 7.4E-6 6.0E-7 C158400700034 13.074 2.7E-5 2.0E-6 C158400700035 ENDDATA 11 0 C158400700036 ENDSUBENT 35 0 C158400799999 SUBENT C1584008 20160318 C158C158400800001 BIB 5 15 C158400800002 REACTION (13-AL-27(A,N)15-P-30,,PY,,TT) C158400800003 METHOD (ACTIV) C158400800004 PART-DET (DG) C158400800005 ERR-ANALYS (DATA-ERR) The uncertainty in the yields is either C158400800006 statistical, due to the number of gamma-ray counts, C158400800007 or set to 7% due to uncertainties in the beam C158400800008 integration, target location, and detector efficiency, C158400800009 whichever is larger. This 7% figure is due to an C158400800010 uncertainty of approximately 5% in bombardment C158400800011 parameters such as current integration and 5% in C158400800012 counting due to source location, and so forth. These C158400800013 uncertainties are then added quadratically. C158400800014 (ERR-1) Bombardment parameters. C158400800015 (ERR-2) Source location. C158400800016 STATUS (TABLE) Table II, page 346. C158400800017 ENDBIB 15 0 C158400800018 COMMON 2 3 C158400800019 ERR-1 ERR-2 C158400800020 PER-CENT PER-CENT C158400800021 5.0 5.0 C158400800022 ENDCOMMON 3 0 C158400800023 DATA 3 17 C158400800024 EN DATA DATA-ERR C158400800025 MEV PRD/INC PRD/INC C158400800026 3.214 2.1E-10 5.0E-11 C158400800027 3.370 2.4E-10 4.0E-11 C158400800028 3.988 1.9E-8 2.0E-9 C158400800029 4.389 3.5E-8 4.0E-9 C158400800030 4.896 2.1E-7 2.0E-8 C158400800031 5.274 4.0E-7 4.0E-8 C158400800032 5.436 5.9E-7 6.0E-8 C158400800033 6.963 4.9E-6 5.0E-7 C158400800034 7.205 5.9E-6 6.0E-7 C158400800035 7.596 8.6E-6 9.0E-7 C158400800036 9.210 1.5E-5 2.0E-6 C158400800037 9.899 3.0E-5 3.0E-6 C158400800038 12.365 2.4E-5 3.0E-6 C158400800039 16.798 5.0E-5 5.0E-6 C158400800040 20.333 6.7E-5 7.0E-6 C158400800041 28.544 8.3E-5 9.0E-6 C158400800042 35.963 1.1E-4 1.0E-5 C158400800043 ENDDATA 19 0 C158400800044 ENDSUBENT 43 0 C158400899999 SUBENT C1584009 20160318 C158C158400900001 BIB 5 15 C158400900002 REACTION (20-CA-40(A,P)21-SC-43,,PY,,TT) C158400900003 METHOD (ACTIV) C158400900004 PART-DET (DG) C158400900005 ERR-ANALYS (DATA-ERR) The uncertainty in the yields is either C158400900006 statistical, due to the number of gamma-ray counts, C158400900007 or set to 7% due to uncertainties in the beam C158400900008 integration, target location, and detector efficiency, C158400900009 whichever is larger. This 7% figure is due to an C158400900010 uncertainty of approximately 5% in bombardment C158400900011 parameters such as current integration and 5% in C158400900012 counting due to source location, and so forth. These C158400900013 uncertainties are then added quadratically. C158400900014 (ERR-1) Bombardment parameters. C158400900015 (ERR-2) Source location. C158400900016 STATUS (TABLE) Table II, page 346. C158400900017 ENDBIB 15 0 C158400900018 COMMON 2 3 C158400900019 ERR-1 ERR-2 C158400900020 PER-CENT PER-CENT C158400900021 5.0 5.0 C158400900022 ENDCOMMON 3 0 C158400900023 DATA 3 23 C158400900024 EN DATA DATA-ERR C158400900025 MEV PRD/INC PRD/INC C158400900026 4.898 8.6E-11 5.0E-11 C158400900027 5.276 9.7E-10 1.0E-10 C158400900028 6.097 2.5E-8 2.0E-9 C158400900029 6.461 8.6E-8 6.0E-9 C158400900030 7.041 4.6E-7 4.0E-8 C158400900031 7.959 2.9E-6 3.0E-7 C158400900032 8.231 3.1E-6 2.0E-7 C158400900033 8.462 4.4E-6 3.0E-7 C158400900034 8.775 6.3E-6 5.0E-7 C158400900035 9.158 9.6E-6 7.0E-7 C158400900036 9.615 1.5E-5 2.0E-6 C158400900037 9.885 1.5E-5 2.0E-6 C158400900038 10.569 2.8E-5 2.0E-6 C158400900039 11.214 3.8E-5 3.0E-6 C158400900040 13.081 1.1E-4 8.0E-6 C158400900041 16.781 2.3E-4 2.0E-5 C158400900042 19.339 3.0E-4 2.0E-5 C158400900043 22.074 3.6E-4 3.0E-5 C158400900044 24.685 4.4E-4 3.0E-5 C158400900045 27.758 4.8E-4 4.0E-5 C158400900046 31.608 5.0E-4 4.0E-5 C158400900047 34.396 5.2E-4 4.0E-5 C158400900048 35.206 5.3E-4 4.0E-5 C158400900049 ENDDATA 25 0 C158400900050 ENDSUBENT 49 0 C158400999999 SUBENT C1584010 20160318 C158C158401000001 BIB 5 15 C158401000002 REACTION (20-CA-48(A,N)22-TI-51,,PY,,TT) C158401000003 METHOD (ACTIV) C158401000004 PART-DET (DG) C158401000005 ERR-ANALYS (DATA-ERR) The uncertainty in the yields is either C158401000006 statistical, due to the number of gamma-ray counts, C158401000007 or set to 7% due to uncertainties in the beam C158401000008 integration, target location, and detector efficiency, C158401000009 whichever is larger. This 7% figure is due to an C158401000010 uncertainty of approximately 5% in bombardment C158401000011 parameters such as current integration and 5% in C158401000012 counting due to source location, and so forth. These C158401000013 uncertainties are then added quadratically. C158401000014 (ERR-1) Bombardment parameters. C158401000015 (ERR-2) Source location. C158401000016 STATUS (TABLE) Table II, page 346. C158401000017 ENDBIB 15 0 C158401000018 COMMON 2 3 C158401000019 ERR-1 ERR-2 C158401000020 PER-CENT PER-CENT C158401000021 5.0 5.0 C158401000022 ENDCOMMON 3 0 C158401000023 DATA 3 16 C158401000024 EN DATA DATA-ERR C158401000025 MEV PRD/INC PRD/INC C158401000026 4.898 3.1E-8 5.0E-9 C158401000027 5.276 3.9E-8 6.0E-9 C158401000028 6.097 2.7E-7 3.0E-8 C158401000029 6.461 6.1E-7 5.0E-8 C158401000030 7.041 2.2E-6 2.0E-7 C158401000031 7.959 8.7E-6 8.0E-7 C158401000032 8.231 1.0E-5 1.0E-6 C158401000033 8.775 1.0E-5 1.0E-6 C158401000034 9.158 1.3E-5 2.0E-6 C158401000035 9.615 1.5E-5 3.0E-6 C158401000036 11.214 2.0E-5 3.0E-6 C158401000037 13.081 3.8E-5 1.0E-5 C158401000038 19.339 6.5E-5 4.0E-4 C158401000039 22.074 7.9E-5 2.0E-4 C158401000040 31.608 1.4E-4 7.0E-5 C158401000041 34.396 8.4E-5 5.0E-5 C158401000042 ENDDATA 18 0 C158401000043 ENDSUBENT 42 0 C158401099999 SUBENT C1584011 20160318 C158C158401100001 BIB 5 15 C158401100002 REACTION (22-TI-46(A,N)24-CR-49,,PY,,TT) C158401100003 METHOD (ACTIV) C158401100004 PART-DET (DG) C158401100005 ERR-ANALYS (DATA-ERR) The uncertainty in the yields is either C158401100006 statistical, due to the number of gamma-ray counts, C158401100007 or set to 7% due to uncertainties in the beam C158401100008 integration, target location, and detector efficiency, C158401100009 whichever is larger. This 7% figure is due to an C158401100010 uncertainty of approximately 5% in bombardment C158401100011 parameters such as current integration and 5% in C158401100012 counting due to source location, and so forth. These C158401100013 uncertainties are then added quadratically. C158401100014 (ERR-1) Bombardment parameters. C158401100015 (ERR-2) Source location. C158401100016 STATUS (TABLE) Table II, page 347. C158401100017 ENDBIB 15 0 C158401100018 COMMON 2 3 C158401100019 ERR-1 ERR-2 C158401100020 PER-CENT PER-CENT C158401100021 5.0 5.0 C158401100022 ENDCOMMON 3 0 C158401100023 DATA 3 24 C158401100024 EN DATA DATA-ERR C158401100025 MEV PRD/INC PRD/INC C158401100026 5.392 1.9E-9 3.0E-10 C158401100027 5.782 1.2E-8 2.0E-9 C158401100028 6.102 3.9E-8 6.0E-9 C158401100029 6.140 1.5E-8 2.0E-9 C158401100030 6.559 8.9E-8 1.0E-8 C158401100031 7.041 3.0E-7 5.0E-8 C158401100032 7.100 4.5E-7 7.0E-8 C158401100033 7.150 4.6E-7 7.0E-8 C158401100034 7.959 1.5E-6 2.0E-7 C158401100035 8.231 2.5E-6 4.0E-7 C158401100036 8.775 4.1E-6 6.0E-7 C158401100037 8.910 6.2E-6 9.0E-7 C158401100038 9.158 5.3E-6 8.0E-7 C158401100039 9.749 9.8E-6 2.0E-6 C158401100040 10.198 1.6E-5 2.0E-6 C158401100041 11.177 2.5E-5 4.0E-6 C158401100042 14.249 7.6E-5 1.0E-5 C158401100043 19.339 1.8E-4 3.0E-5 C158401100044 20.324 2.0E-4 3.0E-5 C158401100045 22.074 2.5E-4 4.0E-5 C158401100046 27.758 3.2E-4 5.0E-5 C158401100047 31.608 5.0E-4 8.0E-5 C158401100048 34.396 5.0E-4 7.0E-5 C158401100049 35.206 4.7E-4 7.0E-5 C158401100050 ENDDATA 26 0 C158401100051 ENDSUBENT 50 0 C158401199999 SUBENT C1584012 20160318 C158C158401200001 BIB 5 15 C158401200002 REACTION (22-TI-48(A,N)24-CR-51,,PY,,TT) C158401200003 METHOD (ACTIV) C158401200004 PART-DET (DG) C158401200005 ERR-ANALYS (DATA-ERR) The uncertainty in the yields is either C158401200006 statistical, due to the number of gamma-ray counts, C158401200007 or set to 7% due to uncertainties in the beam C158401200008 integration, target location, and detector efficiency, C158401200009 whichever is larger. This 7% figure is due to an C158401200010 uncertainty of approximately 5% in bombardment C158401200011 parameters such as current integration and 5% in C158401200012 counting due to source location, and so forth. These C158401200013 uncertainties are then added quadratically. C158401200014 (ERR-1) Bombardment parameters. C158401200015 (ERR-2) Source location. C158401200016 STATUS (TABLE) Table II, page 347. C158401200017 ENDBIB 15 0 C158401200018 COMMON 2 3 C158401200019 ERR-1 ERR-2 C158401200020 PER-CENT PER-CENT C158401200021 5.0 5.0 C158401200022 ENDCOMMON 3 0 C158401200023 DATA 3 24 C158401200024 EN DATA DATA-ERR C158401200025 MEV PRD/INC PRD/INC C158401200026 5.978 7.5E-8 1.0E-8 C158401200027 6.102 1.8E-7 3.0E-8 C158401200028 6.217 2.1E-7 3.0E-8 C158401200029 6.559 4.5E-7 7.0E-8 C158401200030 7.041 1.1E-6 2.0E-7 C158401200031 7.150 1.4E-6 2.0E-7 C158401200032 7.959 4.0E-6 6.0E-7 C158401200033 8.775 1.1E-5 2.0E-6 C158401200034 8.914 1.1E-5 2.0E-6 C158401200035 9.158 1.4E-5 2.0E-6 C158401200036 9.749 2.8E-5 4.0E-6 C158401200037 10.198 2.9E-5 5.0E-6 C158401200038 11.177 6.8E-5 1.0E-5 C158401200039 11.340 4.9E-5 1.0E-5 C158401200040 13.081 1.4E-4 2.0E-5 C158401200041 16.781 3.1E-4 5.0E-5 C158401200042 19.339 4.1E-4 6.0E-5 C158401200043 20.324 4.0E-4 6.0E-5 C158401200044 22.074 4.9E-4 7.0E-5 C158401200045 24.685 4.9E-4 7.0E-5 C158401200046 27.758 5.4E-4 8.0E-5 C158401200047 31.608 5.9E-4 9.0E-5 C158401200048 34.460 5.8E-4 9.0E-5 C158401200049 35.206 6.3E-4 9.0E-5 C158401200050 ENDDATA 26 0 C158401200051 ENDSUBENT 50 0 C158401299999 SUBENT C1584013 20160318 C158C158401300001 BIB 5 15 C158401300002 REACTION (22-TI-49(A,P)23-V-52,,PY,,TT) C158401300003 METHOD (ACTIV) C158401300004 PART-DET (DG) C158401300005 ERR-ANALYS (DATA-ERR) The uncertainty in the yields is either C158401300006 statistical, due to the number of gamma-ray counts, C158401300007 or set to 7% due to uncertainties in the beam C158401300008 integration, target location, and detector efficiency, C158401300009 whichever is larger. This 7% figure is due to an C158401300010 uncertainty of approximately 5% in bombardment C158401300011 parameters such as current integration and 5% in C158401300012 counting due to source location, and so forth. These C158401300013 uncertainties are then added quadratically. C158401300014 (ERR-1) Bombardment parameters. C158401300015 (ERR-2) Source location. C158401300016 STATUS (TABLE) Table II, page 347. C158401300017 ENDBIB 15 0 C158401300018 COMMON 2 3 C158401300019 ERR-1 ERR-2 C158401300020 PER-CENT PER-CENT C158401300021 5.0 5.0 C158401300022 ENDCOMMON 3 0 C158401300023 DATA 3 27 C158401300024 EN DATA DATA-ERR C158401300025 MEV PRD/INC PRD/INC C158401300026 5.781 8.7E-10 2.0E-10 C158401300027 5.978 2.1E-9 3.0E-10 C158401300028 6.120 3.8E-9 6.0E-10 C158401300029 6.217 4.4E-9 7.0E-10 C158401300030 6.471 6.5E-9 1.0E-9 C158401300031 6.559 7.8E-9 1.0E-9 C158401300032 7.041 2.5E-8 4.0E-9 C158401300033 7.104 3.7E-8 6.0E-9 C158401300034 7.390 6.0E-8 9.0E-9 C158401300035 7.959 1.4E-7 2.0E-8 C158401300036 8.231 2.3E-7 4.0E-8 C158401300037 8.775 4.0E-7 6.0E-8 C158401300038 8.914 4.3E-7 7.0E-8 C158401300039 9.158 5.1E-7 8.0E-8 C158401300040 9.749 9.6E-7 2.0E-7 C158401300041 10.198 1.5E-6 2.0E-7 C158401300042 11.340 2.6E-6 4.0E-7 C158401300043 11.391 3.5E-6 5.0E-7 C158401300044 13.081 7.8E-6 1.0E-6 C158401300045 16.786 2.0E-5 3.0E-6 C158401300046 19.339 3.0E-5 5.0E-6 C158401300047 22.074 4.8E-5 7.0E-6 C158401300048 24.685 6.8E-5 1.0E-5 C158401300049 27.758 1.1E-4 2.0E-5 C158401300050 31.608 1.8E-4 3.0E-5 C158401300051 34.396 2.2E-4 3.0E-5 C158401300052 35.206 2.2E-4 3.0E-5 C158401300053 ENDDATA 29 0 C158401300054 ENDSUBENT 53 0 C158401399999 SUBENT C1584014 20160318 C158C158401400001 BIB 5 15 C158401400002 REACTION (22-TI-50(A,P)23-V-53,,PY,,TT) C158401400003 METHOD (ACTIV) C158401400004 PART-DET (DG) C158401400005 ERR-ANALYS (DATA-ERR) The uncertainty in the yields is either C158401400006 statistical, due to the number of gamma-ray counts, C158401400007 or set to 7% due to uncertainties in the beam C158401400008 integration, target location, and detector efficiency, C158401400009 whichever is larger. This 7% figure is due to an C158401400010 uncertainty of approximately 5% in bombardment C158401400011 parameters such as current integration and 5% in C158401400012 counting due to source location, and so forth. These C158401400013 uncertainties are then added quadratically. C158401400014 (ERR-1) Bombardment parameters. C158401400015 (ERR-2) Source location. C158401400016 STATUS (TABLE) Table II, page 347. C158401400017 ENDBIB 15 0 C158401400018 COMMON 2 3 C158401400019 ERR-1 ERR-2 C158401400020 PER-CENT PER-CENT C158401400021 5.0 5.0 C158401400022 ENDCOMMON 3 0 C158401400023 DATA 3 13 C158401400024 EN DATA DATA-ERR C158401400025 MEV PRD/INC PRD/INC C158401400026 8.914 3.3E-8 5.0E-9 C158401400027 11.177 4.4E-7 7.0E-8 C158401400028 11.340 7.1E-7 1.0E-7 C158401400029 13.081 2.0E-6 3.0E-7 C158401400030 13.400 2.8E-6 4.0E-7 C158401400031 16.786 8.2E-6 1.0E-6 C158401400032 19.339 1.6E-5 3.0E-6 C158401400033 20.324 1.7E-5 3.0E-6 C158401400034 22.074 2.3E-5 4.0E-6 C158401400035 24.685 2.5E-5 4.0E-6 C158401400036 27.758 3.0E-5 5.0E-6 C158401400037 31.608 3.6E-5 5.0E-6 C158401400038 34.396 4.1E-5 6.0E-6 C158401400039 ENDDATA 15 0 C158401400040 ENDSUBENT 39 0 C158401499999 SUBENT C1584015 20160318 C158C158401500001 BIB 5 15 C158401500002 REACTION (23-V-51(A,N)25-MN-54,,PY,,TT) C158401500003 METHOD (ACTIV) C158401500004 PART-DET (DG) C158401500005 ERR-ANALYS (DATA-ERR) The uncertainty in the yields is either C158401500006 statistical, due to the number of gamma-ray counts, C158401500007 or set to 7% due to uncertainties in the beam C158401500008 integration, target location, and detector efficiency, C158401500009 whichever is larger. This 7% figure is due to an C158401500010 uncertainty of approximately 5% in bombardment C158401500011 parameters such as current integration and 5% in C158401500012 counting due to source location, and so forth. These C158401500013 uncertainties are then added quadratically. C158401500014 (ERR-1) Bombardment parameters. C158401500015 (ERR-2) Source location. C158401500016 STATUS (TABLE) Table II, page 347. C158401500017 ENDBIB 15 0 C158401500018 COMMON 2 3 C158401500019 ERR-1 ERR-2 C158401500020 PER-CENT PER-CENT C158401500021 5.0 5.0 C158401500022 ENDCOMMON 3 0 C158401500023 DATA 3 12 C158401500024 EN DATA DATA-ERR C158401500025 MEV PRD/INC PRD/INC C158401500026 5.369 5.7E-9 2.0E-9 C158401500027 5.785 2.3E-8 4.0E-9 C158401500028 6.129 4.5E-8 1.0E-8 C158401500029 6.559 2.1E-7 2.0E-8 C158401500030 7.150 9.8E-7 8.0E-8 C158401500031 7.491 2.0E-6 2.0E-8 C158401500032 8.179 5.5E-6 5.0E-7 C158401500033 8.960 1.3E-5 1.0E-6 C158401500034 10.198 4.3E-5 3.0E-6 C158401500035 11.345 8.3E-5 6.0E-6 C158401500036 13.081 1.0E-4 1.0E-5 C158401500037 14.244 2.1E-4 3.0E-5 C158401500038 ENDDATA 14 0 C158401500039 ENDSUBENT 38 0 C158401599999 SUBENT C1584016 20160318 C158C158401600001 BIB 5 15 C158401600002 REACTION (24-CR-50(A,N)26-FE-53,,PY,,TT) C158401600003 METHOD (ACTIV) C158401600004 PART-DET (DG) C158401600005 ERR-ANALYS (DATA-ERR) The uncertainty in the yields is either C158401600006 statistical, due to the number of gamma-ray counts, C158401600007 or set to 7% due to uncertainties in the beam C158401600008 integration, target location, and detector efficiency, C158401600009 whichever is larger. This 7% figure is due to an C158401600010 uncertainty of approximately 5% in bombardment C158401600011 parameters such as current integration and 5% in C158401600012 counting due to source location, and so forth. These C158401600013 uncertainties are then added quadratically. C158401600014 (ERR-1) Bombardment parameters. C158401600015 (ERR-2) Source location. C158401600016 STATUS (TABLE) Table II, page 347. C158401600017 ENDBIB 15 0 C158401600018 COMMON 2 3 C158401600019 ERR-1 ERR-2 C158401600020 PER-CENT PER-CENT C158401600021 5.0 5.0 C158401600022 ENDCOMMON 3 0 C158401600023 DATA 3 24 C158401600024 EN DATA DATA-ERR C158401600025 MEV PRD/INC PRD/INC C158401600026 5.780 6.5E-10 1.0E-10 C158401600027 5.978 1.8E-9 3.0E-10 C158401600028 6.140 3.4E-9 5.0E-10 C158401600029 6.217 3.4E-9 5.0E-10 C158401600030 6.250 5.2E-9 8.0E-10 C158401600031 6.559 1.0E-8 2.0E-9 C158401600032 7.494 1.4E-7 2.0E-8 C158401600033 8.179 4.9E-7 7.0E-8 C158401600034 8.264 5.8E-7 9.0E-8 C158401600035 8.914 1.5E-6 2.0E-7 C158401600036 10.198 5.3E-6 8.0E-7 C158401600037 10.405 5.5E-6 8.0E-7 C158401600038 11.177 9.5E-6 2.0E-6 C158401600039 11.340 1.0E-5 2.0E-6 C158401600040 13.081 2.4E-5 4.0E-6 C158401600041 14.249 3.0E-5 5.0E-6 C158401600042 16.781 4.8E-5 7.0E-6 C158401600043 19.339 7.3E-5 1.0E-5 C158401600044 20.324 7.9E-5 1.0E-5 C158401600045 22.074 8.9E-5 2.0E-5 C158401600046 24.685 9.5E-5 2.0E-5 C158401600047 31.608 1.1E-4 2.0E-5 C158401600048 34.460 1.4E-4 2.0E-5 C158401600049 35.206 1.4E-4 2.0E-5 C158401600050 ENDDATA 26 0 C158401600051 ENDSUBENT 50 0 C158401699999 SUBENT C1584017 20160318 C158C158401700001 BIB 5 15 C158401700002 REACTION (24-CR-53(A,P)25-MN-56,,PY,,TT) C158401700003 METHOD (ACTIV) C158401700004 PART-DET (DG) C158401700005 ERR-ANALYS (DATA-ERR) The uncertainty in the yields is either C158401700006 statistical, due to the number of gamma-ray counts, C158401700007 or set to 7% due to uncertainties in the beam C158401700008 integration, target location, and detector efficiency, C158401700009 whichever is larger. This 7% figure is due to an C158401700010 uncertainty of approximately 5% in bombardment C158401700011 parameters such as current integration and 5% in C158401700012 counting due to source location, and so forth. These C158401700013 uncertainties are then added quadratically. C158401700014 (ERR-1) Bombardment parameters. C158401700015 (ERR-2) Source location. C158401700016 STATUS (TABLE) Table II, page 348. C158401700017 ENDBIB 15 0 C158401700018 COMMON 2 3 C158401700019 ERR-1 ERR-2 C158401700020 PER-CENT PER-CENT C158401700021 5.0 5.0 C158401700022 ENDCOMMON 3 0 C158401700023 DATA 3 18 C158401700024 EN DATA DATA-ERR C158401700025 MEV PRD/INC PRD/INC C158401700026 6.250 1.9E-10 3.0E-11 C158401700027 6.559 5.3E-10 8.0E-11 C158401700028 7.494 1.7E-8 3.0E-9 C158401700029 8.264 7.2E-8 1.0E-8 C158401700030 8.914 2.2E-7 3.0E-8 C158401700031 9.749 6.2E-7 1.0E-7 C158401700032 10.198 9.8E-7 2.0E-7 C158401700033 10.405 1.2E-6 2.0E-7 C158401700034 11.177 2.5E-6 4.0E-7 C158401700035 13.081 8.2E-6 1.0E-6 C158401700036 14.249 1.2E-5 2.0E-6 C158401700037 16.786 2.0E-5 3.0E-6 C158401700038 20.324 3.7E-5 6.0E-6 C158401700039 22.074 4.9E-5 7.0E-6 C158401700040 24.685 6.0E-5 9.0E-6 C158401700041 31.608 9.3E-5 2.0E-5 C158401700042 34.396 1.2E-4 2.0E-5 C158401700043 35.206 1.3E-4 2.0E-5 C158401700044 ENDDATA 20 0 C158401700045 ENDSUBENT 44 0 C158401799999 SUBENT C1584018 20160318 C158C158401800001 BIB 5 15 C158401800002 REACTION (25-MN-55(A,N)27-CO-58,,PY,,TT) C158401800003 METHOD (ACTIV) C158401800004 PART-DET (DG) C158401800005 ERR-ANALYS (DATA-ERR) The uncertainty in the yields is either C158401800006 statistical, due to the number of gamma-ray counts, C158401800007 or set to 7% due to uncertainties in the beam C158401800008 integration, target location, and detector efficiency, C158401800009 whichever is larger. This 7% figure is due to an C158401800010 uncertainty of approximately 5% in bombardment C158401800011 parameters such as current integration and 5% in C158401800012 counting due to source location, and so forth. These C158401800013 uncertainties are then added quadratically. C158401800014 (ERR-1) Bombardment parameters. C158401800015 (ERR-2) Source location. C158401800016 STATUS (TABLE) Table II, page 348. C158401800017 ENDBIB 15 0 C158401800018 COMMON 2 3 C158401800019 ERR-1 ERR-2 C158401800020 PER-CENT PER-CENT C158401800021 5.0 5.0 C158401800022 ENDCOMMON 3 0 C158401800023 DATA 3 21 C158401800024 EN DATA DATA-ERR C158401800025 MEV PRD/INC PRD/INC C158401800026 5.369 1.1E-9 3.0E-10 C158401800027 5.785 5.3E-9 1.0E-10 C158401800028 6.129 1.7E-8 2.0E-9 C158401800029 6.559 7.1E-8 7.0E-9 C158401800030 7.150 3.4E-7 2.0E-8 C158401800031 7.491 7.1E-7 6.0E-8 C158401800032 8.179 2.4E-6 2.0E-7 C158401800033 8.960 6.9E-6 4.0E-7 C158401800034 10.198 2.5E-5 2.0E-6 C158401800035 11.177 4.2E-5 3.0E-6 C158401800036 11.345 4.8E-5 3.0E-6 C158401800037 13.081 1.0E-4 1.0E-5 C158401800038 14.249 1.6E-4 2.0E-5 C158401800039 16.781 2.3E-4 2.0E-5 C158401800040 19.339 2.8E-4 2.0E-5 C158401800041 20.324 3.0E-4 2.0E-5 C158401800042 22.074 3.0E-4 2.0E-5 C158401800043 24.685 3.4E-4 3.0E-5 C158401800044 31.608 3.6E-4 3.0E-5 C158401800045 34.396 3.7E-4 3.0E-5 C158401800046 35.206 3.1E-4 3.0E-5 C158401800047 ENDDATA 23 0 C158401800048 ENDSUBENT 47 0 C158401899999 SUBENT C1584019 20160318 C158C158401900001 BIB 5 15 C158401900002 REACTION (25-MN-55(A,2N)27-CO-57,,PY,,TT) C158401900003 METHOD (ACTIV) C158401900004 PART-DET (DG) C158401900005 ERR-ANALYS (DATA-ERR) The uncertainty in the yields is either C158401900006 statistical, due to the number of gamma-ray counts, C158401900007 or set to 7% due to uncertainties in the beam C158401900008 integration, target location, and detector efficiency, C158401900009 whichever is larger. This 7% figure is due to an C158401900010 uncertainty of approximately 5% in bombardment C158401900011 parameters such as current integration and 5% in C158401900012 counting due to source location, and so forth. These C158401900013 uncertainties are then added quadratically. C158401900014 (ERR-1) Bombardment parameters. C158401900015 (ERR-2) Source location. C158401900016 STATUS (TABLE) Table II, page 348. C158401900017 ENDBIB 15 0 C158401900018 COMMON 2 3 C158401900019 ERR-1 ERR-2 C158401900020 PER-CENT PER-CENT C158401900021 5.0 5.0 C158401900022 ENDCOMMON 3 0 C158401900023 DATA 3 11 C158401900024 EN DATA DATA-ERR C158401900025 MEV PRD/INC PRD/INC C158401900026 13.081 3.0E-7 3.0E-7 C158401900027 14.249 3.4E-6 8.0E-7 C158401900028 16.781 4.0E-5 3.0E-6 C158401900029 19.339 1.3E-4 1.0E-5 C158401900030 20.324 1.6E-4 1.0E-5 C158401900031 22.074 2.6E-4 2.0E-5 C158401900032 24.685 4.1E-4 3.0E-5 C158401900033 27.758 5.9E-4 4.0E-5 C158401900034 31.608 7.7E-4 5.0E-5 C158401900035 34.396 9.2E-4 9.0E-5 C158401900036 35.206 8.2E-4 8.0E-5 C158401900037 ENDDATA 13 0 C158401900038 ENDSUBENT 37 0 C158401999999 SUBENT C1584020 20160318 C158C158402000001 BIB 5 15 C158402000002 REACTION (25-MN-55(A,N+A)25-MN-54,,PY,,TT) C158402000003 METHOD (ACTIV) C158402000004 PART-DET (DG) C158402000005 ERR-ANALYS (DATA-ERR) The uncertainty in the yields is either C158402000006 statistical, due to the number of gamma-ray counts, C158402000007 or set to 7% due to uncertainties in the beam C158402000008 integration, target location, and detector efficiency, C158402000009 whichever is larger. This 7% figure is due to an C158402000010 uncertainty of approximately 5% in bombardment C158402000011 parameters such as current integration and 5% in C158402000012 counting due to source location, and so forth. These C158402000013 uncertainties are then added quadratically. C158402000014 (ERR-1) Bombardment parameters. C158402000015 (ERR-2) Source location. C158402000016 STATUS (TABLE) Table II, page 348. C158402000017 ENDBIB 15 0 C158402000018 COMMON 2 3 C158402000019 ERR-1 ERR-2 C158402000020 PER-CENT PER-CENT C158402000021 5.0 5.0 C158402000022 ENDCOMMON 3 0 C158402000023 DATA 3 8 C158402000024 EN DATA DATA-ERR C158402000025 MEV PRD/INC PRD/INC C158402000026 19.339 1.6E-6 6.0E-7 C158402000027 20.324 2.2E-6 9.0E-7 C158402000028 22.074 6.3E-6 6.0E-7 C158402000029 24.685 2.8E-5 4.0E-6 C158402000030 27.758 8.3E-5 2.0E-5 C158402000031 31.608 1.2E-4 9.0E-6 C158402000032 34.396 2.1E-4 3.0E-5 C158402000033 35.206 2.0E-4 2.0E-5 C158402000034 ENDDATA 10 0 C158402000035 ENDSUBENT 34 0 C158402099999 SUBENT C1584021 20160318 C158C158402100001 BIB 5 15 C158402100002 REACTION (26-FE-54(A,P)27-CO-57,,PY,,TT) C158402100003 METHOD (ACTIV) C158402100004 PART-DET (DG) C158402100005 ERR-ANALYS (DATA-ERR) The uncertainty in the yields is either C158402100006 statistical, due to the number of gamma-ray counts, C158402100007 or set to 7% due to uncertainties in the beam C158402100008 integration, target location, and detector efficiency, C158402100009 whichever is larger. This 7% figure is due to an C158402100010 uncertainty of approximately 5% in bombardment C158402100011 parameters such as current integration and 5% in C158402100012 counting due to source location, and so forth. These C158402100013 uncertainties are then added quadratically. C158402100014 (ERR-1) Bombardment parameters. C158402100015 (ERR-2) Source location. C158402100016 STATUS (TABLE) Table II, page 348. C158402100017 ENDBIB 15 0 C158402100018 COMMON 2 3 C158402100019 ERR-1 ERR-2 C158402100020 PER-CENT PER-CENT C158402100021 5.0 5.0 C158402100022 ENDCOMMON 3 0 C158402100023 DATA 3 12 C158402100024 EN DATA DATA-ERR C158402100025 MEV PRD/INC PRD/INC C158402100026 7.041 7.0E-7 4.0E-7 C158402100027 7.925 2.2E-6 4.0E-7 C158402100028 8.231 6.3E-6 7.0E-7 C158402100029 9.158 1.2E-5 3.0E-6 C158402100030 11.402 2.8E-5 3.0E-6 C158402100031 12.060 3.9E-5 4.0E-6 C158402100032 13.081 7.9E-5 7.0E-6 C158402100033 16.781 2.0E-4 2.0E-5 C158402100034 19.339 3.1E-4 3.0E-5 C158402100035 22.074 4.0E-4 3.0E-5 C158402100036 24.684 4.7E-4 4.0E-5 C158402100037 27.758 4.8E-4 4.0E-5 C158402100038 ENDDATA 14 0 C158402100039 ENDSUBENT 38 0 C158402199999 SUBENT C1584022 20160318 C158C158402200001 BIB 5 15 C158402200002 REACTION (26-FE-54(A,N)28-NI-57,,PY,,TT) C158402200003 METHOD (ACTIV) C158402200004 PART-DET (DG) C158402200005 ERR-ANALYS (DATA-ERR) The uncertainty in the yields is either C158402200006 statistical, due to the number of gamma-ray counts, C158402200007 or set to 7% due to uncertainties in the beam C158402200008 integration, target location, and detector efficiency, C158402200009 whichever is larger. This 7% figure is due to an C158402200010 uncertainty of approximately 5% in bombardment C158402200011 parameters such as current integration and 5% in C158402200012 counting due to source location, and so forth. These C158402200013 uncertainties are then added quadratically. C158402200014 (ERR-1) Bombardment parameters. C158402200015 (ERR-2) Source location. C158402200016 STATUS (TABLE) Table II, page 348. C158402200017 ENDBIB 15 0 C158402200018 COMMON 2 3 C158402200019 ERR-1 ERR-2 C158402200020 PER-CENT PER-CENT C158402200021 5.0 5.0 C158402200022 ENDCOMMON 3 0 C158402200023 DATA 3 16 C158402200024 EN DATA DATA-ERR C158402200025 MEV PRD/INC PRD/INC C158402200026 6.471 2.0E-9 1.0E-9 C158402200027 7.041 2.9E-8 7.0E-9 C158402200028 7.925 1.8E-7 4.0E-8 C158402200029 8.231 3.5E-7 3.0E-8 C158402200030 9.158 1.0E-6 1.0E-7 C158402200031 11.177 7.2E-6 5.0E-7 C158402200032 11.402 7.8E-6 5.0E-7 C158402200033 12.060 1.0E-5 1.0E-6 C158402200034 13.081 1.8E-5 2.0E-6 C158402200035 16.781 4.9E-5 4.0E-6 C158402200036 19.339 7.6E-5 6.0E-6 C158402200037 20.324 9.2E-5 7.0E-6 C158402200038 22.074 9.4E-5 7.0E-6 C158402200039 27.758 1.1E-4 1.0E-5 C158402200040 31.608 1.1E-4 1.0E-5 C158402200041 35.206 1.3E-4 2.0E-5 C158402200042 ENDDATA 18 0 C158402200043 ENDSUBENT 42 0 C158402299999 SUBENT C1584023 20160318 C158C158402300001 BIB 5 15 C158402300002 REACTION (27-CO-59(A,N)29-CU-62,,PY,,TT) C158402300003 METHOD (ACTIV) C158402300004 PART-DET (DG) C158402300005 ERR-ANALYS (DATA-ERR) The uncertainty in the yields is either C158402300006 statistical, due to the number of gamma-ray counts, C158402300007 or set to 7% due to uncertainties in the beam C158402300008 integration, target location, and detector efficiency, C158402300009 whichever is larger. This 7% figure is due to an C158402300010 uncertainty of approximately 5% in bombardment C158402300011 parameters such as current integration and 5% in C158402300012 counting due to source location, and so forth. These C158402300013 uncertainties are then added quadratically. C158402300014 (ERR-1) Bombardment parameters. C158402300015 (ERR-2) Source location. C158402300016 STATUS (TABLE) Table II, page 348. C158402300017 ENDBIB 15 0 C158402300018 COMMON 2 3 C158402300019 ERR-1 ERR-2 C158402300020 PER-CENT PER-CENT C158402300021 5.0 5.0 C158402300022 ENDCOMMON 3 0 C158402300023 DATA 3 17 C158402300024 EN DATA DATA-ERR C158402300025 MEV PRD/INC PRD/INC C158402300026 5.709 1.0E-10 2.0E-11 C158402300027 5.782 1.8E-10 4.0E-11 C158402300028 6.139 1.7E-9 2.0E-11 C158402300029 6.226 2.7E-9 3.0E-10 C158402300030 6.559 9.0E-9 2.0E-9 C158402300031 7.150 7.1E-8 6.0E-9 C158402300032 7.492 1.5E-7 2.0E-8 C158402300033 8.179 6.3E-7 5.0E-8 C158402300034 8.913 2.1E-6 2.0E-7 C158402300035 9.748 7.1E-6 5.0E-7 C158402300036 10.198 1.1E-5 1.0E-6 C158402300037 11.340 2.4E-5 2.0E-6 C158402300038 13.080 5.9E-5 4.0E-6 C158402300039 19.340 1.6E-4 2.0E-5 C158402300040 24.684 3.4E-4 3.0E-5 C158402300041 31.610 3.8E-4 8.0E-5 C158402300042 34.396 3.7E-4 8.0E-5 C158402300043 ENDDATA 19 0 C158402300044 ENDSUBENT 43 0 C158402399999 SUBENT C1584024 20160318 C158C158402400001 BIB 5 15 C158402400002 REACTION (28-NI-58(A,P)29-CU-61,,PY,,TT) C158402400003 METHOD (ACTIV) C158402400004 PART-DET (DG) C158402400005 ERR-ANALYS (DATA-ERR) The uncertainty in the yields is either C158402400006 statistical, due to the number of gamma-ray counts, C158402400007 or set to 7% due to uncertainties in the beam C158402400008 integration, target location, and detector efficiency, C158402400009 whichever is larger. This 7% figure is due to an C158402400010 uncertainty of approximately 5% in bombardment C158402400011 parameters such as current integration and 5% in C158402400012 counting due to source location, and so forth. These C158402400013 uncertainties are then added quadratically. C158402400014 (ERR-1) Bombardment parameters. C158402400015 (ERR-2) Source location. C158402400016 STATUS (TABLE) Table II, page 349. C158402400017 ENDBIB 15 0 C158402400018 COMMON 2 3 C158402400019 ERR-1 ERR-2 C158402400020 PER-CENT PER-CENT C158402400021 5.0 5.0 C158402400022 ENDCOMMON 3 0 C158402400023 DATA 3 22 C158402400024 EN DATA DATA-ERR C158402400025 MEV PRD/INC PRD/INC C158402400026 6.140 1.3E-9 2.0E-10 C158402400027 7.041 1.7E-8 3.0E-9 C158402400028 7.928 1.4E-7 2.0E-8 C158402400029 7.959 1.9E-7 3.0E-8 C158402400030 8.466 5.9E-7 9.0E-8 C158402400031 8.775 6.6E-7 1.0E-7 C158402400032 9.158 1.2E-6 2.0E-7 C158402400033 9.548 3.4E-6 5.0E-7 C158402400034 9.885 4.4E-6 7.0E-7 C158402400035 11.081 2.0E-5 3.0E-6 C158402400036 11.214 1.7E-5 3.0E-6 C158402400037 12.060 3.1E-5 5.0E-6 C158402400038 13.583 5.0E-5 8.0E-6 C158402400039 14.249 8.1E-5 1.0E-5 C158402400040 16.703 1.4E-4 2.0E-5 C158402400041 19.248 2.3E-4 4.0E-5 C158402400042 19.339 2.5E-4 4.0E-5 C158402400043 20.324 2.3E-4 4.0E-5 C158402400044 22.074 2.9E-4 5.0E-5 C158402400045 23.642 3.9E-4 6.0E-5 C158402400046 31.608 4.3E-4 7.0E-5 C158402400047 34.396 5.1E-4 8.0E-5 C158402400048 ENDDATA 24 0 C158402400049 ENDSUBENT 48 0 C158402499999 SUBENT C1584025 20160318 C158C158402500001 BIB 5 15 C158402500002 REACTION (28-NI-60(A,N)30-ZN-63,,PY,,TT) C158402500003 METHOD (ACTIV) C158402500004 PART-DET (DG) C158402500005 ERR-ANALYS (DATA-ERR) The uncertainty in the yields is either C158402500006 statistical, due to the number of gamma-ray counts, C158402500007 or set to 7% due to uncertainties in the beam C158402500008 integration, target location, and detector efficiency, C158402500009 whichever is larger. This 7% figure is due to an C158402500010 uncertainty of approximately 5% in bombardment C158402500011 parameters such as current integration and 5% in C158402500012 counting due to source location, and so forth. These C158402500013 uncertainties are then added quadratically. C158402500014 (ERR-1) Bombardment parameters. C158402500015 (ERR-2) Source location. C158402500016 STATUS (TABLE) Table II, page 349. C158402500017 ENDBIB 15 0 C158402500018 COMMON 2 3 C158402500019 ERR-1 ERR-2 C158402500020 PER-CENT PER-CENT C158402500021 5.0 5.0 C158402500022 ENDCOMMON 3 0 C158402500023 DATA 3 9 C158402500024 EN DATA DATA-ERR C158402500025 MEV PRD/INC PRD/INC C158402500026 9.548 8.4E-7 1.0E-7 C158402500027 9.885 1.7E-6 3.0E-7 C158402500028 10.569 3.0E-6 5.0E-7 C158402500029 11.214 6.4E-6 1.0E-6 C158402500030 13.583 2.7E-5 4.0E-6 C158402500031 14.249 5.5E-5 8.0E-6 C158402500032 16.703 1.0E-4 2.0E-5 C158402500033 19.339 1.5E-4 3.0E-5 C158402500034 22.074 2.1E-4 3.0E-5 C158402500035 ENDDATA 11 0 C158402500036 ENDSUBENT 35 0 C158402599999 SUBENT C1584026 20160318 C158C158402600001 BIB 5 15 C158402600002 REACTION (29-CU-63(A,N)31-GA-66,,PY,,TT) C158402600003 METHOD (ACTIV) C158402600004 PART-DET (DG) C158402600005 ERR-ANALYS (DATA-ERR) The uncertainty in the yields is either C158402600006 statistical, due to the number of gamma-ray counts, C158402600007 or set to 7% due to uncertainties in the beam C158402600008 integration, target location, and detector efficiency, C158402600009 whichever is larger. This 7% figure is due to an C158402600010 uncertainty of approximately 5% in bombardment C158402600011 parameters such as current integration and 5% in C158402600012 counting due to source location, and so forth. These C158402600013 uncertainties are then added quadratically. C158402600014 (ERR-1) Bombardment parameters. C158402600015 (ERR-2) Source location. C158402600016 STATUS (TABLE) Table II, page 349. C158402600017 ENDBIB 15 0 C158402600018 COMMON 2 3 C158402600019 ERR-1 ERR-2 C158402600020 PER-CENT PER-CENT C158402600021 5.0 5.0 C158402600022 ENDCOMMON 3 0 C158402600023 DATA 3 18 C158402600024 EN DATA DATA-ERR C158402600025 MEV PRD/INC PRD/INC C158402600026 8.466 8.6E-8 7.0E-9 C158402600027 8.780 2.1E-7 2.0E-8 C158402600028 8.942 5.9E-7 5.0E-8 C158402600029 9.548 1.8E-6 2.0E-7 C158402600030 9.885 3.0E-6 2.0E-7 C158402600031 10.569 6.0E-6 5.0E-7 C158402600032 11.177 1.1E-5 2.0E-6 C158402600033 11.214 1.3E-5 1.0E-6 C158402600034 11.402 1.4E-5 1.0E-6 C158402600035 12.060 2.1E-5 2.0E-6 C158402600036 13.081 3.4E-5 3.0E-6 C158402600037 13.583 4.8E-5 4.0E-6 C158402600038 16.781 1.4E-4 1.0E-5 C158402600039 19.248 2.2E-4 2.0E-5 C158402600040 19.339 2.1E-4 2.0E-5 C158402600041 20.324 2.4E-4 2.0E-5 C158402600042 22.074 2.4E-4 2.0E-5 C158402600043 24.701 2.8E-4 2.0E-5 C158402600044 ENDDATA 20 0 C158402600045 ENDSUBENT 44 0 C158402699999 SUBENT C1584027 20160318 C158C158402700001 BIB 5 15 C158402700002 REACTION (29-CU-65(A,N)31-GA-68,,PY,,TT) C158402700003 METHOD (ACTIV) C158402700004 PART-DET (DG) C158402700005 ERR-ANALYS (DATA-ERR) The uncertainty in the yields is either C158402700006 statistical, due to the number of gamma-ray counts, C158402700007 or set to 7% due to uncertainties in the beam C158402700008 integration, target location, and detector efficiency, C158402700009 whichever is larger. This 7% figure is due to an C158402700010 uncertainty of approximately 5% in bombardment C158402700011 parameters such as current integration and 5% in C158402700012 counting due to source location, and so forth. These C158402700013 uncertainties are then added quadratically. C158402700014 (ERR-1) Bombardment parameters. C158402700015 (ERR-2) Source location. C158402700016 STATUS (TABLE) Table II, page 349. C158402700017 ENDBIB 15 0 C158402700018 COMMON 2 3 C158402700019 ERR-1 ERR-2 C158402700020 PER-CENT PER-CENT C158402700021 5.0 5.0 C158402700022 ENDCOMMON 3 0 C158402700023 DATA 3 22 C158402700024 EN DATA DATA-ERR C158402700025 MEV PRD/INC PRD/INC C158402700026 6.461 1.4E-9 6.0E-10 C158402700027 7.041 1.6E-8 2.0E-9 C158402700028 7.959 2.3E-7 2.0E-8 C158402700029 8.225 4.8E-7 4.0E-8 C158402700030 8.466 7.5E-7 6.0E-8 C158402700031 8.780 1.2E-6 9.0E-8 C158402700032 8.942 2.0E-6 2.0E-7 C158402700033 9.548 4.5E-6 4.0E-7 C158402700034 9.885 5.7E-6 4.0E-7 C158402700035 10.569 1.2E-5 9.0E-7 C158402700036 11.177 1.9E-5 3.0E-6 C158402700037 11.214 2.3E-5 2.0E-6 C158402700038 12.060 3.5E-5 3.0E-7 C158402700039 13.081 5.6E-5 4.0E-6 C158402700040 13.583 7.0E-5 5.0E-6 C158402700041 14.249 1.1E-4 8.0E-6 C158402700042 16.703 2.1E-4 2.0E-5 C158402700043 19.339 2.9E-4 2.0E-5 C158402700044 20.324 3.2E-4 3.0E-5 C158402700045 24.701 3.7E-4 3.0E-5 C158402700046 31.579 5.1E-4 4.0E-5 C158402700047 34.396 6.0E-4 5.0E-5 C158402700048 ENDDATA 24 0 C158402700049 ENDSUBENT 48 0 C158402799999 SUBENT C1584028 20160318 C158C158402800001 BIB 5 15 C158402800002 REACTION (30-ZN-64(A,P)31-GA-67,,PY,,TT) C158402800003 METHOD (ACTIV) C158402800004 PART-DET (DG) C158402800005 ERR-ANALYS (DATA-ERR) The uncertainty in the yields is either C158402800006 statistical, due to the number of gamma-ray counts, C158402800007 or set to 7% due to uncertainties in the beam C158402800008 integration, target location, and detector efficiency, C158402800009 whichever is larger. This 7% figure is due to an C158402800010 uncertainty of approximately 5% in bombardment C158402800011 parameters such as current integration and 5% in C158402800012 counting due to source location, and so forth. These C158402800013 uncertainties are then added quadratically. C158402800014 (ERR-1) Bombardment parameters. C158402800015 (ERR-2) Source location. C158402800016 STATUS (TABLE) Table II, page 349. C158402800017 ENDBIB 15 0 C158402800018 COMMON 2 3 C158402800019 ERR-1 ERR-2 C158402800020 PER-CENT PER-CENT C158402800021 5.0 5.0 C158402800022 ENDCOMMON 3 0 C158402800023 DATA 3 10 C158402800024 EN DATA DATA-ERR C158402800025 MEV PRD/INC PRD/INC C158402800026 8.026 1.4E-7 2.0E-8 C158402800027 8.876 5.4E-7 6.0E-8 C158402800028 8.880 5.9E-7 6.0E-8 C158402800029 9.899 3.3E-6 5.0E-7 C158402800030 10.170 3.7E-6 6.0E-7 C158402800031 10.380 6.1E-6 8.0E-7 C158402800032 10.400 5.9E-6 8.0E-7 C158402800033 10.680 7.3E-6 1.0E-6 C158402800034 11.840 1.7E-5 3.0E-6 C158402800035 14.244 7.1E-5 2.0E-5 C158402800036 ENDDATA 12 0 C158402800037 ENDSUBENT 36 0 C158402899999 SUBENT C1584029 20160318 C158C158402900001 BIB 5 15 C158402900002 REACTION (30-ZN-64(A,N)32-GE-67,,PY,,TT) C158402900003 METHOD (ACTIV) C158402900004 PART-DET (DG) C158402900005 ERR-ANALYS (DATA-ERR) The uncertainty in the yields is either C158402900006 statistical, due to the number of gamma-ray counts, C158402900007 or set to 7% due to uncertainties in the beam C158402900008 integration, target location, and detector efficiency, C158402900009 whichever is larger. This 7% figure is due to an C158402900010 uncertainty of approximately 5% in bombardment C158402900011 parameters such as current integration and 5% in C158402900012 counting due to source location, and so forth. These C158402900013 uncertainties are then added quadratically. C158402900014 (ERR-1) Bombardment parameters. C158402900015 (ERR-2) Source location. C158402900016 STATUS (TABLE) Table II, page 349. C158402900017 ENDBIB 15 0 C158402900018 COMMON 2 3 C158402900019 ERR-1 ERR-2 C158402900020 PER-CENT PER-CENT C158402900021 5.0 5.0 C158402900022 ENDCOMMON 3 0 C158402900023 DATA 3 9 C158402900024 EN DATA DATA-ERR C158402900025 MEV PRD/INC PRD/INC C158402900026 10.170 2.4E-7 4.0E-8 C158402900027 10.400 3.6E-7 5.0E-8 C158402900028 10.682 6.0E-7 7.0E-8 C158402900029 11.873 3.7E-6 5.0E-7 C158402900030 12.370 5.8E-6 8.0E-7 C158402900031 16.380 3.5E-5 6.0E-6 C158402900032 16.799 3.7E-5 6.0E-6 C158402900033 20.333 8.5E-5 2.0E-5 C158402900034 28.554 1.3E-4 3.0E-5 C158402900035 ENDDATA 11 0 C158402900036 ENDSUBENT 35 0 C158402999999 SUBENT C1584030 20160318 C158C158403000001 BIB 5 15 C158403000002 REACTION (30-ZN-66(A,N)32-GE-69,,PY,,TT) C158403000003 METHOD (ACTIV) C158403000004 PART-DET (DG) C158403000005 ERR-ANALYS (DATA-ERR) The uncertainty in the yields is either C158403000006 statistical, due to the number of gamma-ray counts, C158403000007 or set to 7% due to uncertainties in the beam C158403000008 integration, target location, and detector efficiency, C158403000009 whichever is larger. This 7% figure is due to an C158403000010 uncertainty of approximately 5% in bombardment C158403000011 parameters such as current integration and 5% in C158403000012 counting due to source location, and so forth. These C158403000013 uncertainties are then added quadratically. C158403000014 (ERR-1) Bombardment parameters. C158403000015 (ERR-2) Source location. C158403000016 STATUS (TABLE) Table II, page 349. C158403000017 ENDBIB 15 0 C158403000018 COMMON 2 3 C158403000019 ERR-1 ERR-2 C158403000020 PER-CENT PER-CENT C158403000021 5.0 5.0 C158403000022 ENDCOMMON 3 0 C158403000023 DATA 3 13 C158403000024 EN DATA DATA-ERR C158403000025 MEV PRD/INC PRD/INC C158403000026 8.876 5.8E-7 4.0E-8 C158403000027 9.899 4.2E-6 3.0E-7 C158403000028 10.170 4.9E-6 4.0E-7 C158403000029 10.380 7.6E-6 6.0E-7 C158403000030 10.400 7.7E-6 8.0E-7 C158403000031 10.682 1.0E-5 1.0E-6 C158403000032 11.873 2.5E-5 2.0E-6 C158403000033 11.878 2.7E-5 2.0E-6 C158403000034 12.370 3.2E-5 6.0E-6 C158403000035 14.245 1.0E-4 1.0E-5 C158403000036 16.380 1.1E-4 1.0E-5 C158403000037 20.333 3.5E-4 2.0E-4 C158403000038 28.554 5.9E-4 2.0E-4 C158403000039 ENDDATA 15 0 C158403000040 ENDSUBENT 39 0 C158403099999 SUBENT C1584031 20160318 C158C158403100001 BIB 5 15 C158403100002 REACTION (32-GE-70(A,N)34-SE-73-M,,PY,,TT) C158403100003 METHOD (ACTIV) C158403100004 PART-DET (DG) C158403100005 ERR-ANALYS (DATA-ERR) The uncertainty in the yields is either C158403100006 statistical, due to the number of gamma-ray counts, C158403100007 or set to 7% due to uncertainties in the beam C158403100008 integration, target location, and detector efficiency, C158403100009 whichever is larger. This 7% figure is due to an C158403100010 uncertainty of approximately 5% in bombardment C158403100011 parameters such as current integration and 5% in C158403100012 counting due to source location, and so forth. These C158403100013 uncertainties are then added quadratically. C158403100014 (ERR-1) Bombardment parameters. C158403100015 (ERR-2) Source location. C158403100016 STATUS (TABLE) Table II, page 350. C158403100017 ENDBIB 15 0 C158403100018 COMMON 2 3 C158403100019 ERR-1 ERR-2 C158403100020 PER-CENT PER-CENT C158403100021 5.0 5.0 C158403100022 ENDCOMMON 3 0 C158403100023 DATA 3 17 C158403100024 EN DATA DATA-ERR C158403100025 MEV PRD/INC PRD/INC C158403100026 8.876 1.4E-7 2.0E-8 C158403100027 9.193 4.5E-7 7.0E-8 C158403100028 9.548 1.5E-6 2.0E-7 C158403100029 9.749 1.9E-6 3.0E-7 C158403100030 9.875 2.3E-6 4.0E-7 C158403100031 10.569 6.9E-6 1.0E-6 C158403100032 11.151 1.4E-5 2.0E-6 C158403100033 11.878 2.0E-5 3.0E-6 C158403100034 13.081 4.4E-5 7.0E-6 C158403100035 13.583 5.3E-5 8.0E-6 C158403100036 14.249 8.5E-5 1.0E-5 C158403100037 16.703 1.7E-4 3.0E-5 C158403100038 19.248 2.3E-4 4.0E-5 C158403100039 20.324 2.5E-4 4.0E-5 C158403100040 22.074 3.5E-4 6.0E-5 C158403100041 24.685 4.1E-4 7.0E-5 C158403100042 35.206 4.3E-4 7.0E-5 C158403100043 ENDDATA 19 0 C158403100044 ENDSUBENT 43 0 C158403199999 SUBENT C1584032 20160318 C158C158403200001 BIB 5 15 C158403200002 REACTION (32-GE-72(A,N)34-SE-75,,PY,,TT) C158403200003 METHOD (ACTIV) C158403200004 PART-DET (DG) C158403200005 ERR-ANALYS (DATA-ERR) The uncertainty in the yields is either C158403200006 statistical, due to the number of gamma-ray counts, C158403200007 or set to 7% due to uncertainties in the beam C158403200008 integration, target location, and detector efficiency, C158403200009 whichever is larger. This 7% figure is due to an C158403200010 uncertainty of approximately 5% in bombardment C158403200011 parameters such as current integration and 5% in C158403200012 counting due to source location, and so forth. These C158403200013 uncertainties are then added quadratically. C158403200014 (ERR-1) Bombardment parameters. C158403200015 (ERR-2) Source location. C158403200016 STATUS (TABLE) Table II, page 350. C158403200017 ENDBIB 15 0 C158403200018 COMMON 2 3 C158403200019 ERR-1 ERR-2 C158403200020 PER-CENT PER-CENT C158403200021 5.0 5.0 C158403200022 ENDCOMMON 3 0 C158403200023 DATA 3 20 C158403200024 EN DATA DATA-ERR C158403200025 MEV PRD/INC PRD/INC C158403200026 8.466 2.6E-7 2.0E-8 C158403200027 8.876 5.0E-7 8.0E-8 C158403200028 9.548 1.8E-6 3.0E-7 C158403200029 9.749 2.2E-6 5.0E-7 C158403200030 9.885 2.8E-6 2.0E-7 C158403200031 10.569 5.6E-6 5.0E-7 C158403200032 11.214 1.4E-5 1.0E-6 C158403200033 13.081 5.1E-5 5.0E-6 C158403200034 13.583 5.4E-5 4.0E-6 C158403200035 14.249 7.7E-5 1.0E-5 C158403200036 16.703 1.9E-4 2.0E-5 C158403200037 19.248 2.8E-4 3.0E-5 C158403200038 20.324 3.3E-4 5.0E-5 C158403200039 22.074 4.5E-4 4.0E-5 C158403200040 23.642 4.9E-4 4.0E-5 C158403200041 24.685 5.2E-4 8.0E-5 C158403200042 27.758 6.3E-4 5.0E-5 C158403200043 31.608 8.5E-4 8.0E-5 C158403200044 34.396 9.9E-4 7.0E-5 C158403200045 35.206 1.1E-3 2.0E-4 C158403200046 ENDDATA 22 0 C158403200047 ENDSUBENT 46 0 C158403299999 SUBENT C1584033 20160318 C158C158403300001 BIB 5 15 C158403300002 REACTION (32-GE-74(A,N)34-SE-77-M,,PY,,TT) C158403300003 METHOD (ACTIV) C158403300004 PART-DET (DG) C158403300005 ERR-ANALYS (DATA-ERR) The uncertainty in the yields is either C158403300006 statistical, due to the number of gamma-ray counts, C158403300007 or set to 7% due to uncertainties in the beam C158403300008 integration, target location, and detector efficiency, C158403300009 whichever is larger. This 7% figure is due to an C158403300010 uncertainty of approximately 5% in bombardment C158403300011 parameters such as current integration and 5% in C158403300012 counting due to source location, and so forth. These C158403300013 uncertainties are then added quadratically. C158403300014 (ERR-1) Bombardment parameters. C158403300015 (ERR-2) Source location. C158403300016 STATUS (TABLE) Table II, page 350. C158403300017 ENDBIB 15 0 C158403300018 COMMON 2 3 C158403300019 ERR-1 ERR-2 C158403300020 PER-CENT PER-CENT C158403300021 5.0 5.0 C158403300022 ENDCOMMON 3 0 C158403300023 DATA 3 19 C158403300024 EN DATA DATA-ERR C158403300025 MEV PRD/INC PRD/INC C158403300026 8.231 3.1E-8 5.0E-9 C158403300027 8.466 3.9E-8 6.0E-9 C158403300028 8.775 6.2E-8 1.0E-8 C158403300029 8.876 1.5E-7 2.0E-8 C158403300030 9.193 2.0E-7 3.0E-8 C158403300031 9.749 6.5E-7 1.0E-7 C158403300032 10.198 1.6E-6 2.0E-7 C158403300033 11.214 3.8E-6 6.0E-7 C158403300034 11.800 5.4E-6 8.0E-7 C158403300035 13.081 1.2E-5 2.0E-6 C158403300036 13.583 1.3E-5 2.0E-6 C158403300037 14.249 1.9E-5 3.0E-6 C158403300038 16.703 3.9E-5 6.0E-6 C158403300039 19.248 4.7E-5 7.0E-6 C158403300040 22.074 6.3E-5 1.0E-5 C158403300041 23.642 7.0E-5 1.0E-5 C158403300042 27.758 7.4E-5 1.0E-5 C158403300043 31.608 9.2E-5 2.0E-5 C158403300044 35.206 1.0E-4 2.0E-5 C158403300045 ENDDATA 21 0 C158403300046 ENDSUBENT 45 0 C158403399999 SUBENT C1584034 20160318 C158C158403400001 BIB 5 15 C158403400002 REACTION (32-GE-76(A,N)34-SE-79-M,,PY,,TT) C158403400003 METHOD (ACTIV) C158403400004 PART-DET (DG) C158403400005 ERR-ANALYS (DATA-ERR) The uncertainty in the yields is either C158403400006 statistical, due to the number of gamma-ray counts, C158403400007 or set to 7% due to uncertainties in the beam C158403400008 integration, target location, and detector efficiency, C158403400009 whichever is larger. This 7% figure is due to an C158403400010 uncertainty of approximately 5% in bombardment C158403400011 parameters such as current integration and 5% in C158403400012 counting due to source location, and so forth. These C158403400013 uncertainties are then added quadratically. C158403400014 (ERR-1) Bombardment parameters. C158403400015 (ERR-2) Source location. C158403400016 STATUS (TABLE) Table II, page 350. C158403400017 ENDBIB 15 0 C158403400018 COMMON 2 3 C158403400019 ERR-1 ERR-2 C158403400020 PER-CENT PER-CENT C158403400021 5.0 5.0 C158403400022 ENDCOMMON 3 0 C158403400023 DATA 3 14 C158403400024 EN DATA DATA-ERR C158403400025 MEV PRD/INC PRD/INC C158403400026 7.910 1.9E-9 2.0E-10 C158403400027 8.231 4.3E-9 4.0E-10 C158403400028 8.466 3.1E-8 3.0E-9 C158403400029 8.775 1.1E-8 1.0E-9 C158403400030 9.193 3.1E-8 3.0E-9 C158403400031 9.548 5.8E-8 5.0E-9 C158403400032 9.885 8.2E-8 8.0E-9 C158403400033 10.569 1.8E-7 2.0E-8 C158403400034 10.770 4.0E-7 4.0E-8 C158403400035 11.214 3.7E-7 4.0E-8 C158403400036 13.583 5.4E-7 5.0E-8 C158403400037 16.703 9.0E-7 9.0E-8 C158403400038 19.248 9.7E-7 1.0E-7 C158403400039 23.642 1.5E-6 2.0E-7 C158403400040 ENDDATA 16 0 C158403400041 ENDSUBENT 40 0 C158403499999 SUBENT C1584035 20160318 C158C158403500001 BIB 5 15 C158403500002 REACTION (42-MO-92(A,N)44-RU-95,,PY,,TT) C158403500003 METHOD (ACTIV) C158403500004 PART-DET (DG) C158403500005 ERR-ANALYS (DATA-ERR) The uncertainty in the yields is either C158403500006 statistical, due to the number of gamma-ray counts, C158403500007 or set to 7% due to uncertainties in the beam C158403500008 integration, target location, and detector efficiency, C158403500009 whichever is larger. This 7% figure is due to an C158403500010 uncertainty of approximately 5% in bombardment C158403500011 parameters such as current integration and 5% in C158403500012 counting due to source location, and so forth. These C158403500013 uncertainties are then added quadratically. C158403500014 (ERR-1) Bombardment parameters. C158403500015 (ERR-2) Source location. C158403500016 STATUS (TABLE) Table II, page 350. C158403500017 ENDBIB 15 0 C158403500018 COMMON 2 3 C158403500019 ERR-1 ERR-2 C158403500020 PER-CENT PER-CENT C158403500021 5.0 5.0 C158403500022 ENDCOMMON 3 0 C158403500023 DATA 3 14 C158403500024 EN DATA DATA-ERR C158403500025 MEV PRD/INC PRD/INC C158403500026 9.158 3.4E-10 4.0E-11 C158403500027 9.582 3.1E-9 3.0E-10 C158403500028 9.885 1.7E-8 4.0E-9 C158403500029 10.380 3.4E-8 1.0E-8 C158403500030 10.569 5.3E-8 4.0E-9 C158403500031 11.214 2.4E-7 3.0E-8 C158403500032 11.402 3.0E-7 2.0E-8 C158403500033 11.870 6.6E-7 1.0E-7 C158403500034 13.081 3.9E-6 3.0E-7 C158403500035 14.244 1.0E-5 1.0E-6 C158403500036 16.370 3.2E-5 2.0E-6 C158403500037 16.781 4.7E-5 4.0E-6 C158403500038 19.339 9.6E-5 7.0E-6 C158403500039 22.074 1.7E-4 2.0E-5 C158403500040 ENDDATA 16 0 C158403500041 ENDSUBENT 40 0 C158403599999 SUBENT C1584036 20160318 C158C158403600001 BIB 5 15 C158403600002 REACTION (42-MO-94(A,N)44-RU-97,,PY,,TT) C158403600003 METHOD (ACTIV) C158403600004 PART-DET (DG) C158403600005 ERR-ANALYS (DATA-ERR) The uncertainty in the yields is either C158403600006 statistical, due to the number of gamma-ray counts, C158403600007 or set to 7% due to uncertainties in the beam C158403600008 integration, target location, and detector efficiency, C158403600009 whichever is larger. This 7% figure is due to an C158403600010 uncertainty of approximately 5% in bombardment C158403600011 parameters such as current integration and 5% in C158403600012 counting due to source location, and so forth. These C158403600013 uncertainties are then added quadratically. C158403600014 (ERR-1) Bombardment parameters. C158403600015 (ERR-2) Source location. C158403600016 STATUS (TABLE) Table II, page 350. C158403600017 ENDBIB 15 0 C158403600018 COMMON 2 3 C158403600019 ERR-1 ERR-2 C158403600020 PER-CENT PER-CENT C158403600021 5.0 5.0 C158403600022 ENDCOMMON 3 0 C158403600023 DATA 3 13 C158403600024 EN DATA DATA-ERR C158403600025 MEV PRD/INC PRD/INC C158403600026 9.158 2.2E-10 2.0E-10 C158403600027 9.582 6.0E-9 2.0E-9 C158403600028 9.885 2.3E-8 3.0E-9 C158403600029 10.472 7.2E-8 1.0E-8 C158403600030 11.214 2.5E-7 2.0E-8 C158403600031 11.402 5.2E-7 3.0E-8 C158403600032 11.870 1.3E-6 4.0E-7 C158403600033 13.081 5.5E-6 6.0E-7 C158403600034 14.244 1.3E-5 2.0E-6 C158403600035 16.781 6.1E-5 5.0E-6 C158403600036 19.339 1.3E-4 9.0E-6 C158403600037 22.074 3.3E-4 3.0E-5 C158403600038 24.685 5.1E-4 5.0E-5 C158403600039 ENDDATA 15 0 C158403600040 ENDSUBENT 39 0 C158403699999 SUBENT C1584037 20160318 C158C158403700001 BIB 5 15 C158403700002 REACTION (42-MO-98(A,P)43-TC-101,,PY,,TT) C158403700003 METHOD (ACTIV) C158403700004 PART-DET (DG) C158403700005 ERR-ANALYS (DATA-ERR) The uncertainty in the yields is either C158403700006 statistical, due to the number of gamma-ray counts, C158403700007 or set to 7% due to uncertainties in the beam C158403700008 integration, target location, and detector efficiency, C158403700009 whichever is larger. This 7% figure is due to an C158403700010 uncertainty of approximately 5% in bombardment C158403700011 parameters such as current integration and 5% in C158403700012 counting due to source location, and so forth. These C158403700013 uncertainties are then added quadratically. C158403700014 (ERR-1) Bombardment parameters. C158403700015 (ERR-2) Source location. C158403700016 STATUS (TABLE) Table II, page 350. C158403700017 ENDBIB 15 0 C158403700018 COMMON 2 3 C158403700019 ERR-1 ERR-2 C158403700020 PER-CENT PER-CENT C158403700021 5.0 5.0 C158403700022 ENDCOMMON 3 0 C158403700023 DATA 3 14 C158403700024 EN DATA DATA-ERR C158403700025 MEV PRD/INC PRD/INC C158403700026 7.925 4.0E-12 6.0E-13 C158403700027 8.466 2.3E-11 4.0E-12 C158403700028 8.775 7.4E-11 1.0E-11 C158403700029 9.158 9.7E-11 2.0E-11 C158403700030 9.582 1.0E-10 2.0E-11 C158403700031 9.885 1.2E-10 2.0E-11 C158403700032 10.569 3.6E-10 6.0E-11 C158403700033 11.214 1.2E-9 2.0E-10 C158403700034 11.402 2.3E-9 4.0E-10 C158403700035 13.081 2.0E-8 3.0E-9 C158403700036 16.781 2.6E-7 4.0E-8 C158403700037 19.339 7.8E-7 1.0E-7 C158403700038 22.074 2.2E-6 3.0E-7 C158403700039 24.685 5.4E-6 8.0E-7 C158403700040 ENDDATA 16 0 C158403700041 ENDSUBENT 40 0 C158403799999 SUBENT C1584038 20160318 C158C158403800001 BIB 4 14 C158403800002 REACTION (5-B-10(A,N)7-N-13,,SGV) C158403800003 ANALYSIS The quantity of interest in calculating thermonuclear C158403800004 reaction rates for astrophysical purposes is the C158403800005 product of Avogadro's number with the average value C158403800006 of the cross section times velocity, averaged over a C158403800007 Maxwell-Boltzmann distribution of temperature T. C158403800008 Since this requires extrapolation of the measured C158403800009 yields to form the product integral cross section C158403800010 velocity over the Maxwellian distribution, the rates C158403800011 are quoted over those temperature ranges for which C158403800012 total errors do not exceed 100%. C158403800013 ERR-ANALYS (DATA-ERR) No details on sources of uncertainties. C158403800014 STATUS (TABLE) Table III, page 351. C158403800015 (DEP,C1584002) C158403800016 ENDBIB 14 0 C158403800017 NOCOMMON 0 0 C158403800018 DATA 3 10 C158403800019 KT DATA DATA-ERR C158403800020 K9 CM3/S/MOL PER-CENT C158403800021 3.0 2.0E+4 100. C158403800022 3.5 4.5E+4 100. C158403800023 4.0 9.0E+4 50. C158403800024 4.5 1.6E+5 30. C158403800025 5.0 2.5E+5 25. C158403800026 6.0 5.0E+5 20. C158403800027 7.0 8.0E+5 15. C158403800028 8.0 1.2E+6 15. C158403800029 9.0 1.5E+6 15. C158403800030 10.0 1.9E+6 15. C158403800031 ENDDATA 12 0 C158403800032 ENDSUBENT 31 0 C158403899999 SUBENT C1584039 20160318 C158C158403900001 BIB 4 14 C158403900002 REACTION (7-N-14(A,N)9-F-17,,SGV) C158403900003 ANALYSIS The quantity of interest in calculating thermonuclear C158403900004 reaction rates for astrophysical purposes is the C158403900005 product of Avogadro's number with the average value C158403900006 of the cross section times velocity, averaged over a C158403900007 Maxwell-Boltzmann distribution of temperature T. C158403900008 Since this requires extrapolation of the measured C158403900009 yields to form the product integral cross section C158403900010 velocity over the Maxwellian distribution, the rates C158403900011 are quoted over those temperature ranges for which C158403900012 total errors do not exceed 100%. C158403900013 ERR-ANALYS (DATA-ERR) No details on sources of uncertainties. C158403900014 STATUS (TABLE) Table III, page 351. C158403900015 (DEP,C1584003) C158403900016 ENDBIB 14 0 C158403900017 NOCOMMON 0 0 C158403900018 DATA 3 14 C158403900019 KT DATA DATA-ERR C158403900020 K9 CM3/S/MOL PER-CENT C158403900021 1.0 2.6E-15 15. C158403900022 1.5 7.0E-8 15. C158403900023 2.0 4.0E-4 15. C158403900024 2.5 7.2E-2 15. C158403900025 3.0 2.4E+0 15. C158403900026 3.5 3.0E+1 15. C158403900027 4.0 2.0E+2 15. C158403900028 4.5 9.3E+2 15. C158403900029 5.0 3.1E+3 15. C158403900030 6.0 2.0E+4 15. C158403900031 7.0 7.7E+4 15. C158403900032 8.0 2.1E+5 15. C158403900033 9.0 4.7E+5 20. C158403900034 10.0 8.8E+5 20. C158403900035 ENDDATA 16 0 C158403900036 ENDSUBENT 35 0 C158403999999 SUBENT C1584040 20160318 C158C158404000001 BIB 4 14 C158404000002 REACTION (7-N-15(A,N)9-F-18,,SGV) C158404000003 ANALYSIS The quantity of interest in calculating thermonuclear C158404000004 reaction rates for astrophysical purposes is the C158404000005 product of Avogadro's number with the average value C158404000006 of the cross section times velocity, averaged over a C158404000007 Maxwell-Boltzmann distribution of temperature T. C158404000008 Since this requires extrapolation of the measured C158404000009 yields to form the product integral cross section C158404000010 velocity over the Maxwellian distribution, the rates C158404000011 are quoted over those temperature ranges for which C158404000012 total errors do not exceed 100%. C158404000013 ERR-ANALYS (DATA-ERR) No details on sources of uncertainties. C158404000014 STATUS (TABLE) Table III, page 351. C158404000015 (DEP,C1584005) C158404000016 ENDBIB 14 0 C158404000017 NOCOMMON 0 0 C158404000018 DATA 3 14 C158404000019 KT DATA DATA-ERR C158404000020 K9 CM3/S/MOL PER-CENT C158404000021 1.0 1.2E-24 15. C158404000022 1.5 3.9E-14 15. C158404000023 2.0 6.4E-9 15. C158404000024 2.5 8.2E-6 15. C158404000025 3.0 9.3E-4 15. C158404000026 3.5 2.7E-2 15. C158404000027 4.0 3.3E-1 15. C158404000028 4.5 2.3E+0 15. C158404000029 5.0 1.1E+1 15. C158404000030 6.0 1.0E+2 15. C158404000031 7.0 5.3E+2 15. C158404000032 8.0 1.8E+3 15. C158404000033 9.0 4.6E+3 15. C158404000034 10.0 1.0E+4 15. C158404000035 ENDDATA 16 0 C158404000036 ENDSUBENT 35 0 C158404099999 SUBENT C1584041 20160318 C158C158404100001 BIB 4 14 C158404100002 REACTION (12-MG-25(A,P)13-AL-28,,SGV) C158404100003 ANALYSIS The quantity of interest in calculating thermonuclear C158404100004 reaction rates for astrophysical purposes is the C158404100005 product of Avogadro's number with the average value C158404100006 of the cross section times velocity, averaged over a C158404100007 Maxwell-Boltzmann distribution of temperature T. C158404100008 Since this requires extrapolation of the measured C158404100009 yields to form the product integral cross section C158404100010 velocity over the Maxwellian distribution, the rates C158404100011 are quoted over those temperature ranges for which C158404100012 total errors do not exceed 100%. C158404100013 ERR-ANALYS (DATA-ERR) No details on sources of uncertainties. C158404100014 STATUS (TABLE) Table III, page 351. C158404100015 (DEP,C1584006) C158404100016 ENDBIB 14 0 C158404100017 NOCOMMON 0 0 C158404100018 DATA 3 14 C158404100019 KT DATA DATA-ERR C158404100020 K9 CM3/S/MOL PER-CENT C158404100021 1.0 1.9E-6 90. C158404100022 1.5 1.0E-2 36. C158404100023 2.0 1.2E+0 20. C158404100024 2.5 2.7E+1 15. C158404100025 3.0 2.4E+2 15. C158404100026 3.5 1.3E+3 15. C158404100027 4.0 4.5E+3 15. C158404100028 4.5 1.3E+4 15. C158404100029 5.0 3.1E+4 15. C158404100030 6.0 1.2E+5 15. C158404100031 7.0 3.3E+5 15. C158404100032 8.0 7.1E+5 15. C158404100033 9.0 1.3E+6 15. C158404100034 10.0 2.3E+6 15. C158404100035 ENDDATA 16 0 C158404100036 ENDSUBENT 35 0 C158404199999 SUBENT C1584042 20160318 C158C158404200001 BIB 4 14 C158404200002 REACTION (12-MG-26(A,P)13-AL-29,,SGV) C158404200003 ANALYSIS The quantity of interest in calculating thermonuclear C158404200004 reaction rates for astrophysical purposes is the C158404200005 product of Avogadro's number with the average value C158404200006 of the cross section times velocity, averaged over a C158404200007 Maxwell-Boltzmann distribution of temperature T. C158404200008 Since this requires extrapolation of the measured C158404200009 yields to form the product integral cross section C158404200010 velocity over the Maxwellian distribution, the rates C158404200011 are quoted over those temperature ranges for which C158404200012 total errors do not exceed 100%. C158404200013 ERR-ANALYS (DATA-ERR) No details on sources of uncertainties. C158404200014 STATUS (TABLE) Table III, page 351. C158404200015 (DEP,C1584007) C158404200016 ENDBIB 14 0 C158404200017 NOCOMMON 0 0 C158404200018 DATA 3 14 C158404200019 KT DATA DATA-ERR C158404200020 K9 CM3/S/MOL PER-CENT C158404200021 1.0 2.6E-11 33. C158404200022 1.5 6.9E-6 15. C158404200023 2.0 4.8E-3 15. C158404200024 2.5 2.5E-1 15. C158404200025 3.0 4.3E+0 15. C158404200026 3.5 3.5E+1 15. C158404200027 4.0 1.8E+2 15. C158404200028 4.5 6.5E+2 15. C158404200029 5.0 1.9E+3 15. C158404200030 6.0 9.4E+3 15. C158404200031 7.0 3.1E+4 15. C158404200032 8.0 7.9E+4 15. C158404200033 9.0 1.7E+5 15. C158404200034 10.0 3.0E+5 15. C158404200035 ENDDATA 16 0 C158404200036 ENDSUBENT 35 0 C158404299999 SUBENT C1584043 20160318 C158C158404300001 BIB 4 14 C158404300002 REACTION (13-AL-27(A,N)15-P-30,,SGV) C158404300003 ANALYSIS The quantity of interest in calculating thermonuclear C158404300004 reaction rates for astrophysical purposes is the C158404300005 product of Avogadro's number with the average value C158404300006 of the cross section times velocity, averaged over a C158404300007 Maxwell-Boltzmann distribution of temperature T. C158404300008 Since this requires extrapolation of the measured C158404300009 yields to form the product integral cross section C158404300010 velocity over the Maxwellian distribution, the rates C158404300011 are quoted over those temperature ranges for which C158404300012 total errors do not exceed 100%. C158404300013 ERR-ANALYS (DATA-ERR) No details on sources of uncertainties. C158404300014 STATUS (TABLE) Table III, page 351. C158404300015 (DEP,C1584008) C158404300016 ENDBIB 14 0 C158404300017 NOCOMMON 0 0 C158404300018 DATA 3 14 C158404300019 KT DATA DATA-ERR C158404300020 K9 CM3/S/MOL PER-CENT C158404300021 1.0 2.0E-9 100. C158404300022 1.5 2.7E-4 50. C158404300023 2.0 1.0E-1 15. C158404300024 2.5 4.0E+0 15. C158404300025 3.0 5.0E+1 15. C158404300026 3.5 3.2E+2 15. C158404300027 4.0 1.3E+3 15. C158404300028 4.5 4.0E+3 15. C158404300029 5.0 1.0E+4 15. C158404300030 6.0 4.3E+4 15. C158404300031 7.0 1.3E+5 15. C158404300032 8.0 3.1E+5 15. C158404300033 9.0 6.2E+5 15. C158404300034 10.0 1.1E+6 15. C158404300035 ENDDATA 16 0 C158404300036 ENDSUBENT 35 0 C158404399999 SUBENT C1584044 20160318 C158C158404400001 BIB 4 14 C158404400002 REACTION (20-CA-40(A,P)21-SC-43,,SGV) C158404400003 ANALYSIS The quantity of interest in calculating thermonuclear C158404400004 reaction rates for astrophysical purposes is the C158404400005 product of Avogadro's number with the average value C158404400006 of the cross section times velocity, averaged over a C158404400007 Maxwell-Boltzmann distribution of temperature T. C158404400008 Since this requires extrapolation of the measured C158404400009 yields to form the product integral cross section C158404400010 velocity over the Maxwellian distribution, the rates C158404400011 are quoted over those temperature ranges for which C158404400012 total errors do not exceed 100%. C158404400013 ERR-ANALYS (DATA-ERR) No details on sources of uncertainties. C158404400014 STATUS (TABLE) Table III, page 351. C158404400015 (DEP,C1584009) C158404400016 ENDBIB 14 0 C158404400017 NOCOMMON 0 0 C158404400018 DATA 3 14 C158404400019 KT DATA DATA-ERR C158404400020 K9 CM3/S/MOL PER-CENT C158404400021 1.0 2.9E-17 30. C158404400022 1.5 7.9E-10 15. C158404400023 2.0 6.0E-6 15. C158404400024 2.5 1.6E-3 15. C158404400025 3.0 7.9E-2 15. C158404400026 3.5 1.5E+0 15. C158404400027 4.0 1.4E+1 15. C158404400028 4.5 8.5E+1 15. C158404400029 5.0 3.8E+2 15. C158404400030 6.0 3.7E+3 15. C158404400031 7.0 2.0E+4 15. C158404400032 8.0 7.4E+4 15. C158404400033 9.0 2.1E+5 15. C158404400034 10.0 4.9E+5 15. C158404400035 ENDDATA 16 0 C158404400036 ENDSUBENT 35 0 C158404499999 SUBENT C1584045 20160318 C158C158404500001 BIB 4 14 C158404500002 REACTION (20-CA-48(A,N)22-TI-51,,SGV) C158404500003 ANALYSIS The quantity of interest in calculating thermonuclear C158404500004 reaction rates for astrophysical purposes is the C158404500005 product of Avogadro's number with the average value C158404500006 of the cross section times velocity, averaged over a C158404500007 Maxwell-Boltzmann distribution of temperature T. C158404500008 Since this requires extrapolation of the measured C158404500009 yields to form the product integral cross section C158404500010 velocity over the Maxwellian distribution, the rates C158404500011 are quoted over those temperature ranges for which C158404500012 total errors do not exceed 100%. C158404500013 ERR-ANALYS (DATA-ERR) No details on sources of uncertainties. C158404500014 STATUS (TABLE) Table III, page 351. C158404500015 (DEP,C1584010) C158404500016 ENDBIB 14 0 C158404500017 NOCOMMON 0 0 C158404500018 DATA 3 10 C158404500019 KT DATA DATA-ERR C158404500020 K9 CM3/S/MOL PER-CENT C158404500021 3.0 3.1E+1 100. C158404500022 3.5 6.4E+1 50. C158404500023 4.0 2.4E+2 25. C158404500024 4.5 8.0E+2 20. C158404500025 5.0 2.3E+3 15. C158404500026 6.0 1.3E+4 15. C158404500027 7.0 5.0E+4 15. C158404500028 8.0 1.4E+5 15. C158404500029 9.0 3.3E+5 15. C158404500030 10.0 6.5E+5 15. C158404500031 ENDDATA 12 0 C158404500032 ENDSUBENT 31 0 C158404599999 SUBENT C1584046 20160318 C158C158404600001 BIB 4 14 C158404600002 REACTION (22-TI-46(A,N)24-CR-49,,SGV) C158404600003 ANALYSIS The quantity of interest in calculating thermonuclear C158404600004 reaction rates for astrophysical purposes is the C158404600005 product of Avogadro's number with the average value C158404600006 of the cross section times velocity, averaged over a C158404600007 Maxwell-Boltzmann distribution of temperature T. C158404600008 Since this requires extrapolation of the measured C158404600009 yields to form the product integral cross section C158404600010 velocity over the Maxwellian distribution, the rates C158404600011 are quoted over those temperature ranges for which C158404600012 total errors do not exceed 100%. C158404600013 ERR-ANALYS (DATA-ERR) No details on sources of uncertainties. C158404600014 STATUS (TABLE) Table III, page 351. C158404600015 (DEP,C1584011) C158404600016 ENDBIB 14 0 C158404600017 NOCOMMON 0 0 C158404600018 DATA 3 14 C158404600019 KT DATA DATA-ERR C158404600020 K9 CM3/S/MOL PER-CENT C158404600021 1.0 8.8E-18 100. C158404600022 1.5 4.2E-10 75. C158404600023 2.0 3.5E-6 50. C158404600024 2.5 9.1E-4 30. C158404600025 3.0 4.1E-2 20. C158404600026 3.5 6.9E-1 15. C158404600027 4.0 6.2E+0 15. C158404600028 4.5 3.6E+1 15. C158404600029 5.0 1.5E+2 15. C158404600030 6.0 1.4E+3 15. C158404600031 7.0 7.6E+3 15. C158404600032 8.0 2.8E+4 15. C158404600033 9.0 7.7E+4 15. C158404600034 10.0 1.8E+5 15. C158404600035 ENDDATA 16 0 C158404600036 ENDSUBENT 35 0 C158404699999 SUBENT C1584047 20160318 C158C158404700001 BIB 4 14 C158404700002 REACTION (22-TI-48(A,N)24-CR-51,,SGV) C158404700003 ANALYSIS The quantity of interest in calculating thermonuclear C158404700004 reaction rates for astrophysical purposes is the C158404700005 product of Avogadro's number with the average value C158404700006 of the cross section times velocity, averaged over a C158404700007 Maxwell-Boltzmann distribution of temperature T. C158404700008 Since this requires extrapolation of the measured C158404700009 yields to form the product integral cross section C158404700010 velocity over the Maxwellian distribution, the rates C158404700011 are quoted over those temperature ranges for which C158404700012 total errors do not exceed 100%. C158404700013 ERR-ANALYS (DATA-ERR) No details on sources of uncertainties. C158404700014 STATUS (TABLE) Table III, page 351. C158404700015 (DEP,C1584012) C158404700016 ENDBIB 14 0 C158404700017 NOCOMMON 0 0 C158404700018 DATA 3 14 C158404700019 KT DATA DATA-ERR C158404700020 K9 CM3/S/MOL PER-CENT C158404700021 1.0 1.8E-14 100. C158404700022 1.5 1.9E-8 100. C158404700023 2.0 4.3E-5 100. C158404700024 2.5 6.9E-3 80. C158404700025 3.0 2.6E-1 65. C158404700026 3.5 3.8E+0 50. C158404700027 4.0 3.0E+1 45. C158404700028 4.5 1.6E+2 40. C158404700029 5.0 6.3E+2 25. C158404700030 6.0 5.2E+3 20. C158404700031 7.0 2.5E+4 15. C158404700032 8.0 8.3E+4 15. C158404700033 9.0 2.2E+5 15. C158404700034 10.0 4.9E+5 15. C158404700035 ENDDATA 16 0 C158404700036 ENDSUBENT 35 0 C158404799999 SUBENT C1584048 20160318 C158C158404800001 BIB 4 14 C158404800002 REACTION (22-TI-49(A,P)23-V-52,,SGV) C158404800003 ANALYSIS The quantity of interest in calculating thermonuclear C158404800004 reaction rates for astrophysical purposes is the C158404800005 product of Avogadro's number with the average value C158404800006 of the cross section times velocity, averaged over a C158404800007 Maxwell-Boltzmann distribution of temperature T. C158404800008 Since this requires extrapolation of the measured C158404800009 yields to form the product integral cross section C158404800010 velocity over the Maxwellian distribution, the rates C158404800011 are quoted over those temperature ranges for which C158404800012 total errors do not exceed 100%. C158404800013 ERR-ANALYS (DATA-ERR) No details on sources of uncertainties. C158404800014 STATUS (TABLE) Table III, page 351. C158404800015 (DEP,C1584013) C158404800016 ENDBIB 14 0 C158404800017 NOCOMMON 0 0 C158404800018 DATA 4 12 C158404800019 KT DATA DATA-ERR DATA-ERR C158404800020 K9 CM3/S/MOL PER-CENT PER-CENT C158404800021 2.0 2.1E-7 0.32 32. C158404800022 2.5 6.6E-5 0.17 17. C158404800023 3.0 3.4E-3 0.15 15. C158404800024 3.5 6.2E-2 0.15 15. C158404800025 4.0 5.7E-1 0.15 15. C158404800026 4.5 3.4E+0 0.15 15. C158404800027 5.0 1.4E+1 0.15 15. C158404800028 6.0 1.4E+2 0.15 15. C158404800029 7.0 7.4E+2 0.15 15. C158404800030 8.0 2.7E+3 0.15 15. C158404800031 9.0 7.7E+3 0.15 15. C158404800032 10.0 1.8E+4 0.15 15. C158404800033 ENDDATA 14 0 C158404800034 ENDSUBENT 33 0 C158404899999 SUBENT C1584049 20160318 C158C158404900001 BIB 4 14 C158404900002 REACTION (22-TI-50(A,P)23-V-53,,SGV) C158404900003 ANALYSIS The quantity of interest in calculating thermonuclear C158404900004 reaction rates for astrophysical purposes is the C158404900005 product of Avogadro's number with the average value C158404900006 of the cross section times velocity, averaged over a C158404900007 Maxwell-Boltzmann distribution of temperature T. C158404900008 Since this requires extrapolation of the measured C158404900009 yields to form the product integral cross section C158404900010 velocity over the Maxwellian distribution, the rates C158404900011 are quoted over those temperature ranges for which C158404900012 total errors do not exceed 100%. C158404900013 ERR-ANALYS (DATA-ERR) No details on sources of uncertainties. C158404900014 STATUS (TABLE) Table III, page 351. C158404900015 (DEP,C1584014) C158404900016 ENDBIB 14 0 C158404900017 NOCOMMON 0 0 C158404900018 DATA 3 11 C158404900019 KT DATA DATA-ERR C158404900020 K9 CM3/S/MOL PER-CENT C158404900021 2.5 2.9E-8 60. C158404900022 3.0 4.5E-6 30. C158404900023 3.5 2.0E-4 15. C158404900024 4.0 3.7E-3 15. C158404900025 4.5 3.8E-2 15. C158404900026 5.0 2.5E-1 15. C158404900027 6.0 4.6E+0 15. C158404900028 7.0 3.8E+1 15. C158404900029 8.0 1.9E+2 15. C158404900030 9.0 7.0E+2 15. C158404900031 10.0 2.0E+3 15. C158404900032 ENDDATA 13 0 C158404900033 ENDSUBENT 32 0 C158404999999 SUBENT C1584050 20160318 C158C158405000001 BIB 4 14 C158405000002 REACTION (23-V-51(A,N)25-MN-54,,SGV) C158405000003 ANALYSIS The quantity of interest in calculating thermonuclear C158405000004 reaction rates for astrophysical purposes is the C158405000005 product of Avogadro's number with the average value C158405000006 of the cross section times velocity, averaged over a C158405000007 Maxwell-Boltzmann distribution of temperature T. C158405000008 Since this requires extrapolation of the measured C158405000009 yields to form the product integral cross section C158405000010 velocity over the Maxwellian distribution, the rates C158405000011 are quoted over those temperature ranges for which C158405000012 total errors do not exceed 100%. C158405000013 ERR-ANALYS (DATA-ERR) No details on sources of uncertainties. C158405000014 STATUS (TABLE) Table III, page 351. C158405000015 (DEP,C1584015) C158405000016 ENDBIB 14 0 C158405000017 NOCOMMON 0 0 C158405000018 DATA 3 14 C158405000019 KT DATA DATA-ERR C158405000020 K9 CM3/S/MOL PER-CENT C158405000021 1.0 3.5E-14 83. C158405000022 1.5 1.4E-8 61. C158405000023 2.0 2.3E-5 38. C158405000024 2.5 3.3E-3 21. C158405000025 3.0 1.2E-1 15. C158405000026 3.5 1.8E+0 15. C158405000027 4.0 1.5E+1 15. C158405000028 4.5 8.8E+1 15. C158405000029 5.0 3.7E+2 15. C158405000030 6.0 3.6E+3 15. C158405000031 7.0 2.0E+4 15. C158405000032 8.0 7.2E+4 15. C158405000033 9.0 2.0E+5 15. C158405000034 10.0 4.7E+5 15. C158405000035 ENDDATA 16 0 C158405000036 ENDSUBENT 35 0 C158405099999 SUBENT C1584051 20160318 C158C158405100001 BIB 4 14 C158405100002 REACTION (24-CR-50(A,N)26-FE-53,,SGV) C158405100003 ANALYSIS The quantity of interest in calculating thermonuclear C158405100004 reaction rates for astrophysical purposes is the C158405100005 product of Avogadro's number with the average value C158405100006 of the cross section times velocity, averaged over a C158405100007 Maxwell-Boltzmann distribution of temperature T. C158405100008 Since this requires extrapolation of the measured C158405100009 yields to form the product integral cross section C158405100010 velocity over the Maxwellian distribution, the rates C158405100011 are quoted over those temperature ranges for which C158405100012 total errors do not exceed 100%. C158405100013 ERR-ANALYS (DATA-ERR) No details on sources of uncertainties. C158405100014 STATUS (TABLE) Table III, page 351. C158405100015 (DEP,C1584016) C158405100016 ENDBIB 14 0 C158405100017 NOCOMMON 0 0 C158405100018 DATA 3 14 C158405100019 KT DATA DATA-ERR C158405100020 K9 CM3/S/MOL PER-CENT C158405100021 1.0 1.5E-20 100. C158405100022 1.5 5.6E-12 50. C158405100023 2.0 1.2E-7 30. C158405100024 2.5 5.4E-5 25. C158405100025 3.0 3.5E-3 20. C158405100026 3.5 7.6E-2 15. C158405100027 4.0 8.1E-1 15. C158405100028 4.5 5.4E+0 15. C158405100029 5.0 2.6E+1 15. C158405100030 6.0 2.9E+2 15. C158405100031 7.0 1.8E+3 15. C158405100032 8.0 7.2E+3 15. C158405100033 9.0 2.2E+4 15. C158405100034 10.0 5.4E+4 15. C158405100035 ENDDATA 16 0 C158405100036 ENDSUBENT 35 0 C158405199999 SUBENT C1584052 20160318 C158C158405200001 BIB 4 14 C158405200002 REACTION (24-CR-53(A,P)25-MN-56,,SGV) C158405200003 ANALYSIS The quantity of interest in calculating thermonuclear C158405200004 reaction rates for astrophysical purposes is the C158405200005 product of Avogadro's number with the average value C158405200006 of the cross section times velocity, averaged over a C158405200007 Maxwell-Boltzmann distribution of temperature T. C158405200008 Since this requires extrapolation of the measured C158405200009 yields to form the product integral cross section C158405200010 velocity over the Maxwellian distribution, the rates C158405200011 are quoted over those temperature ranges for which C158405200012 total errors do not exceed 100%. C158405200013 ERR-ANALYS (DATA-ERR) No details on sources of uncertainties. C158405200014 STATUS (TABLE) Table III, page 351. C158405200015 (DEP,C1584017) C158405200016 ENDBIB 14 0 C158405200017 NOCOMMON 0 0 C158405200018 DATA 3 13 C158405200019 KT DATA DATA-ERR C158405200020 K9 CM3/S/MOL PER-CENT C158405200021 1.5 9.2E-14 100. C158405200022 2.0 2.9E-9 45. C158405200023 2.5 2.1E-6 20. C158405200024 3.0 2.0E-4 15. C158405200025 3.5 6.0E-3 15. C158405200026 4.0 7.3E-2 15. C158405200027 4.5 5.9E-1 15. C158405200028 5.0 3.2E+0 15. C158405200029 6.0 4.2E+1 15. C158405200030 7.0 2.9E+2 15. C158405200031 8.0 1.3E+3 15. C158405200032 9.0 4.1E+3 15. C158405200033 10.0 1.1E+4 15. C158405200034 ENDDATA 15 0 C158405200035 ENDSUBENT 34 0 C158405299999 SUBENT C1584053 20160318 C158C158405300001 BIB 4 14 C158405300002 REACTION (25-MN-55(A,N)27-CO-58,,SGV) C158405300003 ANALYSIS The quantity of interest in calculating thermonuclear C158405300004 reaction rates for astrophysical purposes is the C158405300005 product of Avogadro's number with the average value C158405300006 of the cross section times velocity, averaged over a C158405300007 Maxwell-Boltzmann distribution of temperature T. C158405300008 Since this requires extrapolation of the measured C158405300009 yields to form the product integral cross section C158405300010 velocity over the Maxwellian distribution, the rates C158405300011 are quoted over those temperature ranges for which C158405300012 total errors do not exceed 100%. C158405300013 ERR-ANALYS (DATA-ERR) No details on sources of uncertainties. C158405300014 STATUS (TABLE) Table III, page 352. C158405300015 (DEP,C1584018) C158405300016 ENDBIB 14 0 C158405300017 NOCOMMON 0 0 C158405300018 DATA 3 14 C158405300019 KT DATA DATA-ERR C158405300020 K9 CM3/S/MOL PER-CENT C158405300021 1.0 1.7E-16 100. C158405300022 1.5 7.8E-10 100. C158405300023 2.0 3.2E-6 70. C158405300024 2.5 6.8E-4 45. C158405300025 3.0 3.0E-2 25. C158405300026 3.5 5.3E-1 15. C158405300027 4.0 5.1E+0 15. C158405300028 4.5 3.2E+1 15. C158405300029 5.0 1.5E+2 15. C158405300030 6.0 1.6E+3 15. C158405300031 7.0 9.1E+3 15. C158405300032 8.0 3.6E+4 15. C158405300033 9.0 1.1E+5 15. C158405300034 10.0 2.7E+5 15. C158405300035 ENDDATA 16 0 C158405300036 ENDSUBENT 35 0 C158405399999 SUBENT C1584054 20160318 C158C158405400001 BIB 4 14 C158405400002 REACTION (26-FE-54(A,P)27-CO-57,,SGV) C158405400003 ANALYSIS The quantity of interest in calculating thermonuclear C158405400004 reaction rates for astrophysical purposes is the C158405400005 product of Avogadro's number with the average value C158405400006 of the cross section times velocity, averaged over a C158405400007 Maxwell-Boltzmann distribution of temperature T. C158405400008 Since this requires extrapolation of the measured C158405400009 yields to form the product integral cross section C158405400010 velocity over the Maxwellian distribution, the rates C158405400011 are quoted over those temperature ranges for which C158405400012 total errors do not exceed 100%. C158405400013 ERR-ANALYS (DATA-ERR) No details on sources of uncertainties. C158405400014 STATUS (TABLE) Table III, page 352. C158405400015 (DEP,C1584021) C158405400016 ENDBIB 14 0 C158405400017 NOCOMMON 0 0 C158405400018 DATA 3 14 C158405400019 KT DATA DATA-ERR C158405400020 K9 CM3/S/MOL PER-CENT C158405400021 1.0 2.8E-19 15. C158405400022 1.5 2.7E-11 15. C158405400023 2.0 6.4E-7 15. C158405400024 2.5 3.7E-4 15. C158405400025 3.0 3.0E-2 15. C158405400026 3.5 7.2E-1 15. C158405400027 4.0 8.3E+0 15. C158405400028 4.5 5.5E+1 15. C158405400029 5.0 2.6E+2 15. C158405400030 6.0 2.8E+3 15. C158405400031 7.0 1.5E+4 15. C158405400032 8.0 5.4E+4 15. C158405400033 9.0 1.5E+5 15. C158405400034 10.0 3.4E+5 15. C158405400035 ENDDATA 16 0 C158405400036 ENDSUBENT 35 0 C158405499999 SUBENT C1584055 20160318 C158C158405500001 BIB 4 14 C158405500002 REACTION (26-FE-54(A,N)28-NI-57,,SGV) C158405500003 ANALYSIS The quantity of interest in calculating thermonuclear C158405500004 reaction rates for astrophysical purposes is the C158405500005 product of Avogadro's number with the average value C158405500006 of the cross section times velocity, averaged over a C158405500007 Maxwell-Boltzmann distribution of temperature T. C158405500008 Since this requires extrapolation of the measured C158405500009 yields to form the product integral cross section C158405500010 velocity over the Maxwellian distribution, the rates C158405500011 are quoted over those temperature ranges for which C158405500012 total errors do not exceed 100%. C158405500013 ERR-ANALYS (DATA-ERR) No details on sources of uncertainties. C158405500014 STATUS (TABLE) Table III, page 352. C158405500015 (DEP,C1584022) C158405500016 ENDBIB 14 0 C158405500017 NOCOMMON 0 0 C158405500018 DATA 3 14 C158405500019 KT DATA DATA-ERR C158405500020 K9 CM3/S/MOL PER-CENT C158405500021 1.0 1.0E-23 75. C158405500022 1.5 9.1E-14 30. C158405500023 2.0 9.0E-9 20. C158405500024 2.5 9.4E-6 15. C158405500025 3.0 1.0E-3 15. C158405500026 3.5 2.9E-2 15. C158405500027 4.0 3.8E-1 15. C158405500028 4.5 2.8E+0 15. C158405500029 5.0 1.5E+1 15. C158405500030 6.0 1.8E+2 15. C158405500031 7.0 1.1E+3 15. C158405500032 8.0 4.6E+3 15. C158405500033 9.0 1.4E+4 15. C158405500034 10.0 3.7E+4 15. C158405500035 ENDDATA 16 0 C158405500036 ENDSUBENT 35 0 C158405599999 SUBENT C1584056 20160318 C158C158405600001 BIB 4 14 C158405600002 REACTION (27-CO-59(A,N)29-CU-62,,SGV) C158405600003 ANALYSIS The quantity of interest in calculating thermonuclear C158405600004 reaction rates for astrophysical purposes is the C158405600005 product of Avogadro's number with the average value C158405600006 of the cross section times velocity, averaged over a C158405600007 Maxwell-Boltzmann distribution of temperature T. C158405600008 Since this requires extrapolation of the measured C158405600009 yields to form the product integral cross section C158405600010 velocity over the Maxwellian distribution, the rates C158405600011 are quoted over those temperature ranges for which C158405600012 total errors do not exceed 100%. C158405600013 ERR-ANALYS (DATA-ERR) No details on sources of uncertainties. C158405600014 STATUS (TABLE) Table III, page 352. C158405600015 (DEP,C1584023) C158405600016 ENDBIB 14 0 C158405600017 NOCOMMON 0 0 C158405600018 DATA 3 14 C158405600019 KT DATA DATA-ERR C158405600020 K9 CM3/S/MOL PER-CENT C158405600021 1.0 2.9E-21 75. C158405600022 1.5 1.6E-12 35. C158405600023 2.0 5.0E-8 20. C158405600024 2.5 3.1E-5 15. C158405600025 3.0 2.5E-3 15. C158405600026 3.5 6.7E-2 15. C158405600027 4.0 8.4E-1 15. C158405600028 4.5 6.4E+0 15. C158405600029 5.0 3.4E+1 15. C158405600030 6.0 4.6E+2 15. C158405600031 7.0 3.1E+3 15. C158405600032 8.0 1.4E+4 15. C158405600033 9.0 4.5E+4 20. C158405600034 10.0 1.2E+5 30. C158405600035 ENDDATA 16 0 C158405600036 ENDSUBENT 35 0 C158405699999 SUBENT C1584057 20160318 C158C158405700001 BIB 4 14 C158405700002 REACTION (28-NI-58(A,P)29-CU-61,,SGV) C158405700003 ANALYSIS The quantity of interest in calculating thermonuclear C158405700004 reaction rates for astrophysical purposes is the C158405700005 product of Avogadro's number with the average value C158405700006 of the cross section times velocity, averaged over a C158405700007 Maxwell-Boltzmann distribution of temperature T. C158405700008 Since this requires extrapolation of the measured C158405700009 yields to form the product integral cross section C158405700010 velocity over the Maxwellian distribution, the rates C158405700011 are quoted over those temperature ranges for which C158405700012 total errors do not exceed 100%. C158405700013 ERR-ANALYS (DATA-ERR) No details on sources of uncertainties. C158405700014 STATUS (TABLE) Table III, page 352. C158405700015 (DEP,C1584024) C158405700016 ENDBIB 14 0 C158405700017 NOCOMMON 0 0 C158405700018 DATA 3 13 C158405700019 KT DATA DATA-ERR C158405700020 K9 CM3/S/MOL PER-CENT C158405700021 1.5 5.3E-12 100. C158405700022 2.0 6.9E-8 70. C158405700023 2.5 2.6E-5 40. C158405700024 3.0 1.5E-3 30. C158405700025 3.5 3.4E-2 20. C158405700026 4.0 3.9E-1 15. C158405700027 4.5 2.9E+0 15. C158405700028 5.0 1.6E+1 15. C158405700029 6.0 2.2E+2 15. C158405700030 7.0 1.6E+3 15. C158405700031 8.0 7.7E+3 15. C158405700032 9.0 2.7E+4 15. C158405700033 10.0 7.4E+4 15. C158405700034 ENDDATA 15 0 C158405700035 ENDSUBENT 34 0 C158405799999 SUBENT C1584058 20160318 C158C158405800001 BIB 4 14 C158405800002 REACTION (28-NI-60(A,N)30-ZN-63,,SGV) C158405800003 ANALYSIS The quantity of interest in calculating thermonuclear C158405800004 reaction rates for astrophysical purposes is the C158405800005 product of Avogadro's number with the average value C158405800006 of the cross section times velocity, averaged over a C158405800007 Maxwell-Boltzmann distribution of temperature T. C158405800008 Since this requires extrapolation of the measured C158405800009 yields to form the product integral cross section C158405800010 velocity over the Maxwellian distribution, the rates C158405800011 are quoted over those temperature ranges for which C158405800012 total errors do not exceed 100%. C158405800013 ERR-ANALYS (DATA-ERR) No details on sources of uncertainties. C158405800014 STATUS (TABLE) Table III, page 352. C158405800015 (DEP,C1584025) C158405800016 ENDBIB 14 0 C158405800017 NOCOMMON 0 0 C158405800018 DATA 3 13 C158405800019 KT DATA DATA-ERR C158405800020 K9 CM3/S/MOL PER-CENT C158405800021 1.5 7.0E-20 100. C158405800022 2.0 4.4E-13 100. C158405800023 2.5 5.8E-9 80. C158405800024 3.0 3.4E-6 70. C158405800025 3.5 3.3E-4 60. C158405800026 4.0 1.1E-2 50. C158405800027 4.5 1.6E-1 40. C158405800028 5.0 1.3E+0 35. C158405800029 6.0 3.5E+1 30. C158405800030 7.0 3.6E+2 25. C158405800031 8.0 2.1E+3 20. C158405800032 9.0 8.3E+3 20. C158405800033 10.0 2.6E+4 15. C158405800034 ENDDATA 15 0 C158405800035 ENDSUBENT 34 0 C158405899999 SUBENT C1584059 20160318 C158C158405900001 BIB 4 14 C158405900002 REACTION (29-CU-63(A,N)31-GA-66,,SGV) C158405900003 ANALYSIS The quantity of interest in calculating thermonuclear C158405900004 reaction rates for astrophysical purposes is the C158405900005 product of Avogadro's number with the average value C158405900006 of the cross section times velocity, averaged over a C158405900007 Maxwell-Boltzmann distribution of temperature T. C158405900008 Since this requires extrapolation of the measured C158405900009 yields to form the product integral cross section C158405900010 velocity over the Maxwellian distribution, the rates C158405900011 are quoted over those temperature ranges for which C158405900012 total errors do not exceed 100%. C158405900013 ERR-ANALYS (DATA-ERR) No details on sources of uncertainties. C158405900014 STATUS (TABLE) Table III, page 352. C158405900015 (DEP,C1584026) C158405900016 ENDBIB 14 0 C158405900017 NOCOMMON 0 0 C158405900018 DATA 3 13 C158405900019 KT DATA DATA-ERR C158405900020 K9 CM3/S/MOL PER-CENT C158405900021 1.5 1.9E-18 100. C158405900022 2.0 5.4E-12 100. C158405900023 2.5 4.5E-8 75. C158405900024 3.0 1.9E-5 60. C158405900025 3.5 1.5E-3 50. C158405900026 4.0 3.8E-2 45. C158405900027 4.5 4.9E-1 40. C158405900028 5.0 3.8E+0 30. C158405900029 6.0 8.4E+1 25. C158405900030 7.0 7.8E+2 20. C158405900031 8.0 4.2E+3 15. C158405900032 9.0 1.6E+4 15. C158405900033 10.0 4.6E+4 15. C158405900034 ENDDATA 15 0 C158405900035 ENDSUBENT 34 0 C158405999999 SUBENT C1584060 20160318 C158C158406000001 BIB 4 14 C158406000002 REACTION (29-CU-65(A,N)31-GA-68,,SGV) C158406000003 ANALYSIS The quantity of interest in calculating thermonuclear C158406000004 reaction rates for astrophysical purposes is the C158406000005 product of Avogadro's number with the average value C158406000006 of the cross section times velocity, averaged over a C158406000007 Maxwell-Boltzmann distribution of temperature T. C158406000008 Since this requires extrapolation of the measured C158406000009 yields to form the product integral cross section C158406000010 velocity over the Maxwellian distribution, the rates C158406000011 are quoted over those temperature ranges for which C158406000012 total errors do not exceed 100%. C158406000013 ERR-ANALYS (DATA-ERR) No details on sources of uncertainties. C158406000014 STATUS (TABLE) Table III, page 352. C158406000015 (DEP,C1584027) C158406000016 ENDBIB 14 0 C158406000017 NOCOMMON 0 0 C158406000018 DATA 3 14 C158406000019 KT DATA DATA-ERR C158406000020 K9 CM3/S/MOL PER-CENT C158406000021 1.0 2.9E-24 75. C158406000022 1.5 4.0E-14 30. C158406000023 2.0 4.4E-9 20. C158406000024 2.5 5.3E-6 15. C158406000025 3.0 6.7E-4 15. C158406000026 3.5 2.3E-2 15. C158406000027 4.0 3.5E-1 15. C158406000028 4.5 3.1E+0 15. C158406000029 5.0 1.8E+1 15. C158406000030 6.0 2.8E+2 15. C158406000031 7.0 2.1E+3 15. C158406000032 8.0 1.0E+4 15. C158406000033 9.0 3.5E+4 15. C158406000034 10.0 9.5E+4 15. C158406000035 ENDDATA 16 0 C158406000036 ENDSUBENT 35 0 C158406099999 SUBENT C1584061 20160318 C158C158406100001 BIB 4 14 C158406100002 REACTION (30-ZN-64(A,P)31-GA-67,,SGV) C158406100003 ANALYSIS The quantity of interest in calculating thermonuclear C158406100004 reaction rates for astrophysical purposes is the C158406100005 product of Avogadro's number with the average value C158406100006 of the cross section times velocity, averaged over a C158406100007 Maxwell-Boltzmann distribution of temperature T. C158406100008 Since this requires extrapolation of the measured C158406100009 yields to form the product integral cross section C158406100010 velocity over the Maxwellian distribution, the rates C158406100011 are quoted over those temperature ranges for which C158406100012 total errors do not exceed 100%. C158406100013 ERR-ANALYS (DATA-ERR) No details on sources of uncertainties. C158406100014 STATUS (TABLE) Table III, page 352. C158406100015 (DEP,C1584028) C158406100016 ENDBIB 14 0 C158406100017 NOCOMMON 0 0 C158406100018 DATA 3 14 C158406100019 KT DATA DATA-ERR C158406100020 K9 CM3/S/MOL PER-CENT C158406100021 1.0 4.7E-24 100. C158406100022 1.5 8.5E-15 90. C158406100023 2.0 7.1E-10 80. C158406100024 2.5 8.6E-7 70. C158406100025 3.0 1.1E-4 60. C158406100026 3.5 3.8E-3 50. C158406100027 4.0 5.4E-2 40. C158406100028 4.5 4.2E-1 35. C158406100029 5.0 2.2E+0 30. C158406100030 6.0 2.6E+1 25. C158406100031 7.0 1.4E+2 20. C158406100032 8.0 5.1E+2 20. C158406100033 9.0 1.4E+3 15. C158406100034 10.0 2.9E+3 15. C158406100035 ENDDATA 16 0 C158406100036 ENDSUBENT 35 0 C158406199999 SUBENT C1584062 20160318 C158C158406200001 BIB 4 14 C158406200002 REACTION (30-ZN-64(A,N)32-GE-67,,SGV) C158406200003 ANALYSIS The quantity of interest in calculating thermonuclear C158406200004 reaction rates for astrophysical purposes is the C158406200005 product of Avogadro's number with the average value C158406200006 of the cross section times velocity, averaged over a C158406200007 Maxwell-Boltzmann distribution of temperature T. C158406200008 Since this requires extrapolation of the measured C158406200009 yields to form the product integral cross section C158406200010 velocity over the Maxwellian distribution, the rates C158406200011 are quoted over those temperature ranges for which C158406200012 total errors do not exceed 100%. C158406200013 ERR-ANALYS (DATA-ERR) No details on sources of uncertainties. C158406200014 STATUS (TABLE) Table III, page 352. C158406200015 (DEP,C1584029) C158406200016 ENDBIB 14 0 C158406200017 NOCOMMON 0 0 C158406200018 DATA 3 13 C158406200019 KT DATA DATA-ERR C158406200020 K9 CM3/S/MOL PER-CENT C158406200021 1.5 1.1E-23 40. C158406200022 2.0 7.8E-16 25. C158406200023 2.5 3.7E-11 20. C158406200024 3.0 4.9E-8 20. C158406200025 3.5 8.5E-6 15. C158406200026 4.0 4.0E-4 15. C158406200027 4.5 8.3E-3 15. C158406200028 5.0 9.3E-2 15. C158406200029 6.0 3.6E+0 15. C158406200030 7.0 4.9E+1 15. C158406200031 8.0 3.6E+2 15. C158406200032 9.0 1.7E+3 15. C158406200033 10.0 5.9E+3 15. C158406200034 ENDDATA 15 0 C158406200035 ENDSUBENT 34 0 C158406299999 SUBENT C1584063 20160318 C158C158406300001 BIB 4 14 C158406300002 REACTION (30-ZN-66(A,N)32-GE-69,,SGV) C158406300003 ANALYSIS The quantity of interest in calculating thermonuclear C158406300004 reaction rates for astrophysical purposes is the C158406300005 product of Avogadro's number with the average value C158406300006 of the cross section times velocity, averaged over a C158406300007 Maxwell-Boltzmann distribution of temperature T. C158406300008 Since this requires extrapolation of the measured C158406300009 yields to form the product integral cross section C158406300010 velocity over the Maxwellian distribution, the rates C158406300011 are quoted over those temperature ranges for which C158406300012 total errors do not exceed 100%. C158406300013 ERR-ANALYS (DATA-ERR) No details on sources of uncertainties. C158406300014 STATUS (TABLE) Table III, page 352. C158406300015 (DEP,C1584030) C158406300016 ENDBIB 14 0 C158406300017 NOCOMMON 0 0 C158406300018 DATA 3 13 C158406300019 KT DATA DATA-ERR C158406300020 K9 CM3/S/MOL PER-CENT C158406300021 1.5 3.0E-18 100. C158406300022 2.0 6.5E-12 100. C158406300023 2.5 4.9E-8 70. C158406300024 3.0 2.0E-5 50. C158406300025 3.5 1.5E-3 40. C158406300026 4.0 3.9E-2 25. C158406300027 4.5 5.1E-1 25. C158406300028 5.0 4.0E+0 20. C158406300029 6.0 9.2E+1 15. C158406300030 7.0 8.9E+2 15. C158406300031 8.0 5.0E+3 15. C158406300032 9.0 1.9E+4 15. C158406300033 10.0 5.7E+4 15. C158406300034 ENDDATA 15 0 C158406300035 ENDSUBENT 34 0 C158406399999 SUBENT C1584064 20160318 C158C158406400001 BIB 4 14 C158406400002 REACTION (32-GE-70(A,N)34-SE-73-M,,SGV) C158406400003 ANALYSIS The quantity of interest in calculating thermonuclear C158406400004 reaction rates for astrophysical purposes is the C158406400005 product of Avogadro's number with the average value C158406400006 of the cross section times velocity, averaged over a C158406400007 Maxwell-Boltzmann distribution of temperature T. C158406400008 Since this requires extrapolation of the measured C158406400009 yields to form the product integral cross section C158406400010 velocity over the Maxwellian distribution, the rates C158406400011 are quoted over those temperature ranges for which C158406400012 total errors do not exceed 100%. C158406400013 ERR-ANALYS (DATA-ERR) No details on sources of uncertainties. C158406400014 STATUS (TABLE) Table III, page 352. C158406400015 (DEP,C1584031) C158406400016 ENDBIB 14 0 C158406400017 NOCOMMON 0 0 C158406400018 DATA 3 13 C158406400019 KT DATA DATA-ERR C158406400020 K9 CM3/S/MOL PER-CENT C158406400021 1.5 4.2E-18 100. C158406400022 2.0 3.6E-12 80. C158406400023 2.5 2.2E-8 75. C158406400024 3.0 8.8E-6 60. C158406400025 3.5 7.1E-4 40. C158406400026 4.0 2.0E-2 30. C158406400027 4.5 2.7E-1 25. C158406400028 5.0 2.3E+0 20. C158406400029 6.0 5.7E+1 15. C158406400030 7.0 5.9E+2 15. C158406400031 8.0 3.4E+3 15. C158406400032 9.0 1.4E+4 15. C158406400033 10.0 4.3E+4 15. C158406400034 ENDDATA 15 0 C158406400035 ENDSUBENT 34 0 C158406499999 SUBENT C1584065 20160318 C158C158406500001 BIB 4 14 C158406500002 REACTION (32-GE-72(A,N)34-SE-75,,SGV) C158406500003 ANALYSIS The quantity of interest in calculating thermonuclear C158406500004 reaction rates for astrophysical purposes is the C158406500005 product of Avogadro's number with the average value C158406500006 of the cross section times velocity, averaged over a C158406500007 Maxwell-Boltzmann distribution of temperature T. C158406500008 Since this requires extrapolation of the measured C158406500009 yields to form the product integral cross section C158406500010 velocity over the Maxwellian distribution, the rates C158406500011 are quoted over those temperature ranges for which C158406500012 total errors do not exceed 100%. C158406500013 ERR-ANALYS (DATA-ERR) No details on sources of uncertainties. C158406500014 STATUS (TABLE) Table III, page 352. C158406500015 (DEP,C1584032) C158406500016 ENDBIB 14 0 C158406500017 NOCOMMON 0 0 C158406500018 DATA 3 14 C158406500019 KT DATA DATA-ERR C158406500020 K9 CM3/S/MOL PER-CENT C158406500021 1.0 4.9E-28 100. C158406500022 1.5 6.6E-17 100. C158406500023 2.0 4.0E-11 80. C158406500024 2.5 1.6E-7 75. C158406500025 3.0 4.4E-5 60. C158406500026 3.5 2.6E-3 50. C158406500027 4.0 5.8E-2 45. C158406500028 4.5 6.7E-1 35. C158406500029 5.0 4.8E+0 30. C158406500030 6.0 9.5E+1 25. C158406500031 7.0 8.4E+2 15. C158406500032 8.0 4.4E+3 15. C158406500033 9.0 1.7E+4 15. C158406500034 10.0 4.9E+4 15. C158406500035 ENDDATA 16 0 C158406500036 ENDSUBENT 35 0 C158406599999 SUBENT C1584066 20160318 C158C158406600001 BIB 4 14 C158406600002 REACTION (32-GE-74(A,N)34-SE-77-M,,SGV) C158406600003 ANALYSIS The quantity of interest in calculating thermonuclear C158406600004 reaction rates for astrophysical purposes is the C158406600005 product of Avogadro's number with the average value C158406600006 of the cross section times velocity, averaged over a C158406600007 Maxwell-Boltzmann distribution of temperature T. C158406600008 Since this requires extrapolation of the measured C158406600009 yields to form the product integral cross section C158406600010 velocity over the Maxwellian distribution, the rates C158406600011 are quoted over those temperature ranges for which C158406600012 total errors do not exceed 100%. C158406600013 ERR-ANALYS (DATA-ERR) No details on sources of uncertainties. C158406600014 STATUS (TABLE) Table III, page 352. C158406600015 (DEP,C1584033) C158406600016 ENDBIB 14 0 C158406600017 NOCOMMON 0 0 C158406600018 DATA 3 14 C158406600019 KT DATA DATA-ERR C158406600020 K9 CM3/S/MOL PER-CENT C158406600021 1.0 4.3E-25 100. C158406600022 1.5 6.9E-16 100. C158406600023 2.0 6.3E-11 100. C158406600024 2.5 9.8E-8 100. C158406600025 3.0 1.8E-5 75. C158406600026 3.5 8.4E-4 60. C158406600027 4.0 1.7E-2 50. C158406600028 4.5 1.8E-1 35. C158406600029 5.0 1.3E+0 25. C158406600030 6.0 2.5E+1 15. C158406600031 7.0 2.3E+2 15. C158406600032 8.0 1.2E+3 15. C158406600033 9.0 4.6E+3 15. C158406600034 10.0 1.4E+4 15. C158406600035 ENDDATA 16 0 C158406600036 ENDSUBENT 35 0 C158406699999 SUBENT C1584067 20160318 C158C158406700001 BIB 4 14 C158406700002 REACTION (32-GE-76(A,N)34-SE-79-M,,SGV) C158406700003 ANALYSIS The quantity of interest in calculating thermonuclear C158406700004 reaction rates for astrophysical purposes is the C158406700005 product of Avogadro's number with the average value C158406700006 of the cross section times velocity, averaged over a C158406700007 Maxwell-Boltzmann distribution of temperature T. C158406700008 Since this requires extrapolation of the measured C158406700009 yields to form the product integral cross section C158406700010 velocity over the Maxwellian distribution, the rates C158406700011 are quoted over those temperature ranges for which C158406700012 total errors do not exceed 100%. C158406700013 ERR-ANALYS (DATA-ERR) No details on sources of uncertainties. C158406700014 STATUS (TABLE) Table III, page 353. C158406700015 (DEP,C1584034) C158406700016 ENDBIB 14 0 C158406700017 NOCOMMON 0 0 C158406700018 DATA 3 10 C158406700019 KT DATA DATA-ERR C158406700020 K9 CM3/S/MOL PER-CENT C158406700021 3.0 3.0E-5 100. C158406700022 3.5 4.0E-4 100. C158406700023 4.0 4.3E-3 100. C158406700024 4.5 3.6E-2 75. C158406700025 5.0 2.2E-1 70. C158406700026 6.0 3.6E+0 50. C158406700027 7.0 2.9E+1 15. C158406700028 8.0 1.4E+2 15. C158406700029 9.0 4.9E+2 15. C158406700030 10.0 1.3E+3 15. C158406700031 ENDDATA 12 0 C158406700032 ENDSUBENT 31 0 C158406799999 SUBENT C1584068 20160318 C158C158406800001 BIB 4 14 C158406800002 REACTION (42-MO-92(A,N)44-RU-95,,SGV) C158406800003 ANALYSIS The quantity of interest in calculating thermonuclear C158406800004 reaction rates for astrophysical purposes is the C158406800005 product of Avogadro's number with the average value C158406800006 of the cross section times velocity, averaged over a C158406800007 Maxwell-Boltzmann distribution of temperature T. C158406800008 Since this requires extrapolation of the measured C158406800009 yields to form the product integral cross section C158406800010 velocity over the Maxwellian distribution, the rates C158406800011 are quoted over those temperature ranges for which C158406800012 total errors do not exceed 100%. C158406800013 ERR-ANALYS (DATA-ERR) No details on sources of uncertainties. C158406800014 STATUS (TABLE) Table III, page 353. C158406800015 (DEP,C1584035) C158406800016 ENDBIB 14 0 C158406800017 NOCOMMON 0 0 C158406800018 DATA 3 13 C158406800019 KT DATA DATA-ERR C158406800020 K9 CM3/S/MOL PER-CENT C158406800021 1.5 1.6E-23 50. C158406800022 2.0 3.4E-16 25. C158406800023 2.5 8.9E-12 15. C158406800024 3.0 8.7E-9 15. C158406800025 3.5 1.3E-6 15. C158406800026 4.0 5.8E-5 15. C158406800027 4.5 1.2E-3 15. C158406800028 5.0 1.4E-2 15. C158406800029 6.0 6.1E-1 15. C158406800030 7.0 1.0E+1 15. C158406800031 8.0 8.5E+1 15. C158406800032 9.0 4.7E+2 15. C158406800033 10.0 1.9E+3 15. C158406800034 ENDDATA 15 0 C158406800035 ENDSUBENT 34 0 C158406899999 SUBENT C1584069 20160318 C158C158406900001 BIB 4 14 C158406900002 REACTION (42-MO-94(A,N)44-RU-97,,SGV) C158406900003 ANALYSIS The quantity of interest in calculating thermonuclear C158406900004 reaction rates for astrophysical purposes is the C158406900005 product of Avogadro's number with the average value C158406900006 of the cross section times velocity, averaged over a C158406900007 Maxwell-Boltzmann distribution of temperature T. C158406900008 Since this requires extrapolation of the measured C158406900009 yields to form the product integral cross section C158406900010 velocity over the Maxwellian distribution, the rates C158406900011 are quoted over those temperature ranges for which C158406900012 total errors do not exceed 100%. C158406900013 ERR-ANALYS (DATA-ERR) No details on sources of uncertainties. C158406900014 STATUS (TABLE) Table III, page 353. C158406900015 (DEP,C1584036) C158406900016 ENDBIB 14 0 C158406900017 NOCOMMON 0 0 C158406900018 DATA 3 13 C158406900019 KT DATA DATA-ERR C158406900020 K9 CM3/S/MOL PER-CENT C158406900021 1.5 1.9E-23 40. C158406900022 2.0 4.4E-16 20. C158406900023 2.5 1.3E-11 15. C158406900024 3.0 1.3E-8 15. C158406900025 3.5 1.9E-6 15. C158406900026 4.0 8.9E-5 15. C158406900027 4.5 1.8E-3 15. C158406900028 5.0 2.1E-2 15. C158406900029 6.0 9.3E-1 15. C158406900030 7.0 1.5E+1 15. C158406900031 8.0 1.2E+2 15. C158406900032 9.0 6.7E+2 15. C158406900033 10.0 2.7E+3 25. C158406900034 ENDDATA 15 0 C158406900035 ENDSUBENT 34 0 C158406999999 SUBENT C1584070 20160318 C158C158407000001 BIB 4 14 C158407000002 REACTION (42-MO-98(A,P)43-TC-101,,SGV) C158407000003 ANALYSIS The quantity of interest in calculating thermonuclear C158407000004 reaction rates for astrophysical purposes is the C158407000005 product of Avogadro's number with the average value C158407000006 of the cross section times velocity, averaged over a C158407000007 Maxwell-Boltzmann distribution of temperature T. C158407000008 Since this requires extrapolation of the measured C158407000009 yields to form the product integral cross section C158407000010 velocity over the Maxwellian distribution, the rates C158407000011 are quoted over those temperature ranges for which C158407000012 total errors do not exceed 100%. C158407000013 ERR-ANALYS (DATA-ERR) No details on sources of uncertainties. C158407000014 STATUS (TABLE) Table III, page 353. C158407000015 (DEP,C1584037) C158407000016 ENDBIB 14 0 C158407000017 NOCOMMON 0 0 C158407000018 DATA 3 13 C158407000019 KT DATA DATA-ERR C158407000020 K9 CM3/S/MOL PER-CENT C158407000021 1.5 7.5E-21 100. C158407000022 2.0 5.6E-15 70. C158407000023 2.5 2.1E-11 60. C158407000024 3.0 5.2E-9 50. C158407000025 3.5 2.8E-7 40. C158407000026 4.0 5.7E-6 30. C158407000027 4.5 6.2E-5 25. C158407000028 5.0 4.4E-4 20. C158407000029 6.0 9.3E-3 15. C158407000030 7.0 9.6E-2 15. C158407000031 8.0 6.3E-1 15. C158407000032 9.0 2.9E+0 15. C158407000033 10.0 1.1E+1 15. C158407000034 ENDDATA 15 0 C158407000035 ENDSUBENT 34 0 C158407099999 ENDENTRY 70 0 C158499999999