ENTRY C2309 20230112 C230900000001 SUBENT C2309001 20230112 20240316 C230900100001 BIB 9 32 C230900100002 TITLE Spallation-fission competition in heavy-element C230900100003 reactions: Th232+He4 and U233+d C230900100004 AUTHOR (B.M.Foreman Jr,W.M.Gibson,R.A.Glass,G.T.Seaborg) C230900100005 REFERENCE (J,PR,116,382,1959) C230900100006 #doi:10.1103/physrev.116.382 C230900100007 (R,UCRL-3493,1956) Preliminary U233 report data. C230900100008 REL-REF (O,C2882001,W.M.Gibson+,R,UCRL-3493,1956) Related C230900100009 Pu239 and Np237 data from Berkeley report. C230900100010 INSTITUTE (1USABRK,1USAUCX) C230900100011 FACILITY (CYCLO,1USABRK) Berkeley 60-inch cyclotron. C230900100012 DETECTOR (PROPC) C230900100013 METHOD (CHSEP,ACTIV) For the thorium foil bombardments the C230900100014 large amounts of activity produced allowed separate C230900100015 aliquots of the dissolved target to Be used for the C230900100016 various fractions analyzed. For the thorium C230900100017 bombardments the protactinium fraction was purified C230900100018 by extraction with diisopropyl ketone (dipk) and C230900100019 elution on an anion-exchange column. The uranium C230900100020 fraction was purified by an anion-exchange-column C230900100021 elution. For the U233 bombardments the chemical C230900100022 separation of the neptunium fraction was described by C230900100023 vandenbosch. The protactinium fraction was separated C230900100024 from the neptunium by carrying neptunium (iv) C230900100025 fluoride on laf3. the counting rates of C230900100026 alpha-particle-emitting spallation products were C230900100027 measured by use of a multichannel alpha-pulse-height C230900100028 analyzer. The counting rates of spallation products C230900100029 which decay by orbital electron capture were C230900100030 determined with a methane-flow windowless C230900100031 proportional counter. C230900100032 HISTORY (20180601C) BP C230900100033 (20230112A) BP: Added REL-REF and Berkeley report. C230900100034 ENDBIB 32 0 C230900100035 COMMON 1 3 C230900100036 EN-ERR C230900100037 MEV C230900100038 0.5 C230900100039 ENDCOMMON 3 0 C230900100040 ENDSUBENT 39 0 C230900199999 SUBENT C2309002 20180815 C177C230900200001 BIB 6 15 C230900200002 REACTION (90-TH-232(A,4N)92-U-232,,SIG) Spallation product. C230900200003 SAMPLE A few of the thorium targets were thin uniform depositsC230900200004 (~500 microg/cm2) of the hydrated thorium or uranium C230900200005 oxide electrodeposited on aluminum. The amount of C230900200006 Th232 was determined by alpha counting of the C230900200007 resulting thin deposits. C230900200008 ERR-ANALYS (DATA-ERR) The limits of spallation errors are C230900200009 estimated. The quoted limits of error in the C230900200010 spallation cross sections do not include C230900200011 uncertainties in the counting efficiencies used. C230900200012 DECAY-DATA (92-U-232,70.0YR,A) C230900200013 CORRECTION For thorium, corrections were applied to account for C230900200014 the contribution from alpha particle-emitting C230900200015 daughters of the Th232. C230900200016 STATUS (TABLE) Table I, page 384. C230900200017 ENDBIB 15 0 C230900200018 NOCOMMON 0 0 C230900200019 DATA 5 15 C230900200020 EN-MIN EN-MAX DATA DATA-ERR DATA-MAX C230900200021 MEV MEV MB MB MB C230900200022 25.7 28.9 0.008 C230900200023 29.9 31.8 0.11 0.06 C230900200024 30.6 33.4 1. 0.1 C230900200025 32.0 33.7 0.12 0.01 C230900200026 34.8 36.9 17.9 1.8 C230900200027 34.9 37.7 15.6 1.6 C230900200028 34.9 37.7 19. 1.9 C230900200029 35.8 37.8 17.5 1.8 C230900200030 39.0 41.6 54.5 5.5 C230900200031 39.3 41.0 54.7 5.5 C230900200032 43.4 45.9 3.7 1. C230900200033 43.4 45.9 34.7 3.7 C230900200034 43.4 45.9 33.4 3.3 C230900200035 43.4 45.9 100.0 C230900200036 43.8 45.4 31.6 3.2 C230900200037 ENDDATA 17 0 C230900200038 ENDSUBENT 37 0 C230900299999 SUBENT C2309003 20180815 C177C230900300001 BIB 6 15 C230900300002 REACTION (90-TH-232(A,5N)92-U-231,,SIG) Spallation product. C230900300003 SAMPLE A few of the thorium targets were thin uniform depositsC230900300004 (~500 microg/cm2) of the hydrated thorium or uranium C230900300005 oxide electrodeposited on aluminum. The amount of C230900300006 Th232 was determined by alpha counting of the C230900300007 resulting thin deposits. C230900300008 ERR-ANALYS (DATA-ERR) The limits of spallation errors are C230900300009 estimated. The quoted limits of error in the C230900300010 spallation cross sections do not include C230900300011 uncertainties in the counting efficiencies used. C230900300012 DECAY-DATA (92-U-231,4.3D,A) C230900300013 CORRECTION For thorium, corrections were applied to account for C230900300014 the contribution from alpha particle-emitting C230900300015 daughters of the Th232. C230900300016 STATUS (TABLE) Table I, page 384. C230900300017 ENDBIB 15 0 C230900300018 NOCOMMON 0 0 C230900300019 DATA 4 1 C230900300020 EN-MIN EN-MAX DATA DATA-ERR C230900300021 MEV MEV MB MB C230900300022 43.4 45.9 3.7 1.0 C230900300023 ENDDATA 3 0 C230900300024 ENDSUBENT 23 0 C230900399999 SUBENT C2309004 20180815 C177C230900400001 BIB 6 15 C230900400002 REACTION (90-TH-232(A,P)91-PA-235,,SIG) Spallation product. C230900400003 SAMPLE A few of the thorium targets were thin uniform depositsC230900400004 (~500 microg/cm2) of the hydrated thorium or uranium C230900400005 oxide electrodeposited on aluminum. The amount of C230900400006 Th232 was determined by alpha counting of the C230900400007 resulting thin deposits. C230900400008 ERR-ANALYS (DATA-ERR) The limits of spallation errors are C230900400009 estimated. The quoted limits of error in the C230900400010 spallation cross sections do not include C230900400011 uncertainties in the counting efficiencies used. C230900400012 DECAY-DATA (91-PA-235,23.7MIN,B-) C230900400013 CORRECTION For thorium, corrections were applied to account for C230900400014 the contribution from alpha particle-emitting C230900400015 daughters of the Th232. C230900400016 STATUS (TABLE) Table I, page 384. C230900400017 ENDBIB 15 0 C230900400018 NOCOMMON 0 0 C230900400019 DATA 5 9 C230900400020 EN-MIN EN-MAX DATA DATA-ERR DATA-MAX C230900400021 MEV MEV MB MB MB C230900400022 21.6 23.9 0.07 C230900400023 25.7 28.1 1.14 0.4 C230900400024 27.6 29.9 0.64 0.21 C230900400025 29.9 31.8 3.4 0.6 C230900400026 32.0 33.7 3.3 1.2 C230900400027 34.8 36.9 2.9 0.6 C230900400028 35.8 37.8 5.4 2.0 C230900400029 39.3 41.0 3.0 1.5 C230900400030 43.8 45.4 1.7 C230900400031 ENDDATA 11 0 C230900400032 ENDSUBENT 31 0 C230900499999 SUBENT C2309005 20180815 C177C230900500001 BIB 6 15 C230900500002 REACTION (90-TH-232(A,X)91-PA-234-G,CUM,SIG) Spallation product.C230900500003 SAMPLE A few of the thorium targets were thin uniform depositsC230900500004 (~500 microg/cm2) of the hydrated thorium or uranium C230900500005 oxide electrodeposited on aluminum. The amount of C230900500006 Th232 was determined by alpha counting of the C230900500007 resulting thin deposits. C230900500008 ERR-ANALYS (DATA-ERR) The limits of spallation errors are C230900500009 estimated. The quoted limits of error in the C230900500010 spallation cross sections do not include C230900500011 uncertainties in the counting efficiencies used. C230900500012 DECAY-DATA (91-PA-234-G,6.7HR,B-) C230900500013 CORRECTION For thorium, corrections were applied to account for C230900500014 the contribution from alpha particle-emitting C230900500015 daughters of the Th232. C230900500016 STATUS (TABLE) Table I, page 384. C230900500017 ENDBIB 15 0 C230900500018 NOCOMMON 0 0 C230900500019 DATA 4 10 C230900500020 EN-MIN EN-MAX DATA DATA-ERR C230900500021 MEV MEV MB MB C230900500022 25.7 28.1 0.61 0.2 C230900500023 27.6 29.9 0.41 0.04 C230900500024 29.9 31.8 5.2 0.5 C230900500025 32.0 33.7 6.4 0.6 C230900500026 34.8 36.9 16.0 2.0 C230900500027 35.8 37.8 21.0 2.0 C230900500028 39.0 41.6 21.0 2.0 C230900500029 39.3 41.0 22.0 2.0 C230900500030 43.4 45.9 18.0 2.0 C230900500031 43.8 45.4 19.0 4.0 C230900500032 ENDDATA 12 0 C230900500033 ENDSUBENT 32 0 C230900599999 SUBENT C2309006 20180815 C177C230900600001 BIB 6 15 C230900600002 REACTION (90-TH-232(A,X)91-PA-233,CUM,SIG) Spallation product. C230900600003 SAMPLE A few of the thorium targets were thin uniform depositsC230900600004 (~500 microg/cm2) of the hydrated thorium or uranium C230900600005 oxide electrodeposited on aluminum. The amount of C230900600006 Th232 was determined by alpha counting of the C230900600007 resulting thin deposits. C230900600008 ERR-ANALYS (DATA-ERR) The limits of spallation errors are C230900600009 estimated. The quoted limits of error in the C230900600010 spallation cross sections do not include C230900600011 uncertainties in the counting efficiencies used. C230900600012 DECAY-DATA (91-PA-233,27.0D,B-) C230900600013 CORRECTION For thorium, corrections were applied to account for C230900600014 the contribution from alpha particle-emitting C230900600015 daughters of the Th232. C230900600016 STATUS (TABLE) Table I, page 384. C230900600017 ENDBIB 15 0 C230900600018 NOCOMMON 0 0 C230900600019 DATA 4 14 C230900600020 EN-MIN EN-MAX DATA DATA-ERR C230900600021 MEV MEV MB MB C230900600022 15.0 18.0 0.21 0.02 C230900600023 19.9 22.4 0.21 0.03 C230900600024 21.6 23.9 0.41 0.05 C230900600025 23.6 25.9 0.31 0.05 C230900600026 25.7 28.1 3.3 0.4 C230900600027 27.6 29.9 2.4 0.3 C230900600028 29.9 31.8 8.5 0.9 C230900600029 32.0 33.7 10.0 1.0 C230900600030 34.8 36.9 14.0 2.0 C230900600031 35.8 37.8 17.0 2.0 C230900600032 39.0 41.6 18.0 2.0 C230900600033 39.3 41.0 21.0 2.0 C230900600034 43.4 45.9 22.0 3.0 C230900600035 43.8 45.4 24.0 5.0 C230900600036 ENDDATA 16 0 C230900600037 ENDSUBENT 36 0 C230900699999 SUBENT C2309007 20180815 C177C230900700001 BIB 6 15 C230900700002 REACTION (90-TH-232(A,X)91-PA-232,,SIG) Spallation product. C230900700003 SAMPLE A few of the thorium targets were thin uniform depositsC230900700004 (~500 microg/cm2) of the hydrated thorium or uranium C230900700005 oxide electrodeposited on aluminum. The amount of C230900700006 Th232 was determined by alpha counting of the C230900700007 resulting thin deposits. C230900700008 ERR-ANALYS (DATA-ERR) The limits of spallation errors are C230900700009 estimated. The quoted limits of error in the C230900700010 spallation cross sections do not include C230900700011 uncertainties in the counting efficiencies used. C230900700012 DECAY-DATA (91-PA-232,1.31D,B-) C230900700013 CORRECTION For thorium, corrections were applied to account for C230900700014 the contribution from alpha particle-emitting C230900700015 daughters of the Th232. C230900700016 STATUS (TABLE) Table I, page 384. C230900700017 ENDBIB 15 0 C230900700018 NOCOMMON 0 0 C230900700019 DATA 4 11 C230900700020 EN-MIN EN-MAX DATA DATA-ERR C230900700021 MEV MEV MB MB C230900700022 15.0 18.0 0.11 0.002 C230900700023 19.9 22.4 0.016 0.03 C230900700024 21.6 23.9 0.02 0.006 C230900700025 27.6 29.9 0.08 0.02 C230900700026 29.9 31.8 0.34 0.1 C230900700027 32.0 33.7 0.25 0.05 C230900700028 34.8 36.9 0.93 0.2 C230900700029 35.8 37.8 1.8 0.4 C230900700030 39.3 41.0 2.3 0.4 C230900700031 43.4 45.9 5.2 1.1 C230900700032 43.8 45.4 4.1 1.0 C230900700033 ENDDATA 13 0 C230900700034 ENDSUBENT 33 0 C230900799999 SUBENT C2309008 20180815 C177C230900800001 BIB 6 15 C230900800002 REACTION (90-TH-232(A,2P)90-TH-234,,SIG) Spallation product. C230900800003 SAMPLE A few of the thorium targets were thin uniform depositsC230900800004 (~500 microg/cm2) of the hydrated thorium or uranium C230900800005 oxide electrodeposited on aluminum. The amount of C230900800006 Th232 was determined by alpha counting of the C230900800007 resulting thin deposits. C230900800008 ERR-ANALYS (DATA-ERR) The limits of spallation errors are C230900800009 estimated. The quoted limits of error in the C230900800010 spallation cross sections do not include C230900800011 uncertainties in the counting efficiencies used. C230900800012 DECAY-DATA (90-TH-234,24.1D,B-) C230900800013 CORRECTION For thorium, corrections were applied to account for C230900800014 the contribution from alpha particle-emitting C230900800015 daughters of the Th232. C230900800016 STATUS (TABLE) Table I, page 384. C230900800017 ENDBIB 15 0 C230900800018 NOCOMMON 0 0 C230900800019 DATA 5 6 C230900800020 EN-MIN EN-MAX DATA DATA-ERR DATA-MAX C230900800021 MEV MEV MB MB MB C230900800022 25.7 28.1 0.16 0.08 C230900800023 29.9 31.8 0.055 0.028 C230900800024 30.6 33.4 0.01 C230900800025 32.0 33.7 0.08 C230900800026 39.0 41.6 6.0 C230900800027 43.4 45.9 0.07 C230900800028 ENDDATA 8 0 C230900800029 ENDSUBENT 28 0 C230900899999 SUBENT C2309009 20180815 C177C230900900001 BIB 6 15 C230900900002 REACTION (90-TH-232(A,X)90-TH-233,CUM,SIG) Spallation product. C230900900003 SAMPLE A few of the thorium targets were thin uniform depositsC230900900004 (~500 microg/cm2) of the hydrated thorium or uranium C230900900005 oxide electrodeposited on aluminum. The amount of C230900900006 Th232 was determined by alpha counting of the C230900900007 resulting thin deposits. C230900900008 ERR-ANALYS (DATA-ERR) The limits of spallation errors are C230900900009 estimated. The quoted limits of error in the C230900900010 spallation cross sections do not include C230900900011 uncertainties in the counting efficiencies used. C230900900012 DECAY-DATA (90-TH-233,23.3MIN,B-) C230900900013 CORRECTION For thorium, corrections were applied to account for C230900900014 the contribution from alpha particle-emitting C230900900015 daughters of the Th232. C230900900016 STATUS (TABLE) Table I, page 384. C230900900017 ENDBIB 15 0 C230900900018 NOCOMMON 0 0 C230900900019 DATA 5 9 C230900900020 EN-MIN EN-MAX DATA DATA-ERR DATA-MAX C230900900021 MEV MEV MB MB MB C230900900022 19.9 22.4 0.11 0.06 C230900900023 21.6 23.9 0.14 C230900900024 25.7 28.1 0.54 0.27 C230900900025 29.9 31.8 0.62 0.31 C230900900026 32.0 33.7 2.9 1.1 C230900900027 34.8 36.9 0.36 0.19 C230900900028 35.8 37.8 1.9 1.4 C230900900029 39.3 41.0 2.0 0.7 C230900900030 43.8 45.4 4.2 1.5 C230900900031 ENDDATA 11 0 C230900900032 ENDSUBENT 31 0 C230900999999 SUBENT C2309010 20180815 C177C230901000001 BIB 6 15 C230901000002 REACTION (90-TH-232(A,X)90-TH-231,CUM,SIG) Spallation product. C230901000003 SAMPLE A few of the thorium targets were thin uniform depositsC230901000004 (~500 microg/cm2) of the hydrated thorium or uranium C230901000005 oxide electrodeposited on aluminum. The amount of C230901000006 Th232 was determined by alpha counting of the C230901000007 resulting thin deposits. C230901000008 ERR-ANALYS (DATA-ERR) The limits of spallation errors are C230901000009 estimated. The quoted limits of error in the C230901000010 spallation cross sections do not include C230901000011 uncertainties in the counting efficiencies used. C230901000012 DECAY-DATA (90-TH-231,25.6HR,B-) C230901000013 CORRECTION For thorium, corrections were applied to account for C230901000014 the contribution from alpha particle-emitting C230901000015 daughters of the Th232. C230901000016 STATUS (TABLE) Table I, page 384. C230901000017 ENDBIB 15 0 C230901000018 NOCOMMON 0 0 C230901000019 DATA 5 17 C230901000020 EN-MIN EN-MAX DATA DATA-ERR DATA-MAX C230901000021 MEV MEV MB MB MB C230901000022 15.0 18.0 3.6 1.2 C230901000023 19.9 22.4 0.93 0.4 C230901000024 21.6 23.9 0.14 C230901000025 25.7 28.1 0.84 0.28 C230901000026 27.6 29.9 3.6 1.2 C230901000027 29.9 31.8 2.3 0.8 C230901000028 30.6 33.4 1.5 0.6 C230901000029 34.8 36.9 16.0 2.0 C230901000030 34.9 37.7 20.0 4.0 C230901000031 34.9 37.7 12.0 3.0 C230901000032 35.8 37.8 28.0 7.0 C230901000033 39.0 41.6 37.0 19.0 C230901000034 39.3 41.0 15.0 5.0 C230901000035 39.6 42.2 31.0 6.0 C230901000036 43.4 45.9 42.0 8.0 C230901000037 43.4 45.9 49.0 14.0 C230901000038 43.8 45.4 35.0 9.0 C230901000039 ENDDATA 19 0 C230901000040 ENDSUBENT 39 0 C230901099999 SUBENT C2309011 20180815 C177C230901100001 BIB 6 13 C230901100002 REACTION (90-TH-232(A,4N)92-U-232,,SIG) Spallation product. C230901100003 SAMPLE An electroplated target. The amount of C230901100004 Th232 was determined by alpha counting of the C230901100005 resulting thin deposits. C230901100006 ERR-ANALYS (DATA-ERR) The limits of spallation errors are C230901100007 estimated. The quoted limits of error in the C230901100008 spallation cross sections do not include C230901100009 uncertainties in the counting efficiencies used. C230901100010 DECAY-DATA (92-U-232,70.0YR,A) C230901100011 CORRECTION For thorium, corrections were applied to account for C230901100012 the contribution from alpha particle-emitting C230901100013 daughters of the Th232. C230901100014 STATUS (TABLE) Table I, page 384. C230901100015 ENDBIB 13 0 C230901100016 NOCOMMON 0 0 C230901100017 DATA 4 2 C230901100018 EN DATA DATA-ERR DATA-MAX C230901100019 MEV MB MB MB C230901100020 32.3 30.0 C230901100021 38.9 27.9 2.8 C230901100022 ENDDATA 4 0 C230901100023 ENDSUBENT 22 0 C230901199999 SUBENT C2309012 20180815 C177C230901200001 BIB 5 9 C230901200002 REACTION (90-TH-232(A,2P)90-TH-234,,SIG) Spallation product. C230901200003 SAMPLE An electroplated target. The amount of C230901200004 Th232 was determined by alpha counting of the C230901200005 resulting thin deposits. C230901200006 DECAY-DATA (90-TH-234,24.1D,B-) C230901200007 CORRECTION For thorium, corrections were applied to account for C230901200008 the contribution from alpha particle-emitting C230901200009 daughters of the Th232. C230901200010 STATUS (TABLE) Table I, page 384. C230901200011 ENDBIB 9 0 C230901200012 NOCOMMON 0 0 C230901200013 DATA 2 2 C230901200014 EN DATA-MAX C230901200015 MEV MB C230901200016 26.5 2.1 C230901200017 35.9 0.2 C230901200018 ENDDATA 4 0 C230901200019 ENDSUBENT 18 0 C230901299999 SUBENT C2309013 20180815 C177C230901300001 BIB 6 13 C230901300002 REACTION (90-TH-232(A,X)90-TH-231,CUM,SIG) Spallation product C230901300003 SAMPLE An electroplated target. The amount of C230901300004 Th232 was determined by alpha counting of the C230901300005 resulting thin deposits. C230901300006 ERR-ANALYS (DATA-ERR) The limits of spallation errors are C230901300007 estimated. The quoted limits of error in the C230901300008 spallation cross sections do not include C230901300009 uncertainties in the counting efficiencies used. C230901300010 DECAY-DATA (90-TH-231,25.6HR,B-) C230901300011 CORRECTION For thorium, corrections were applied to account for C230901300012 the contribution from alpha particle-emitting C230901300013 daughters of the Th232. C230901300014 STATUS (TABLE) Table I, page 384. C230901300015 ENDBIB 13 0 C230901300016 NOCOMMON 0 0 C230901300017 DATA 4 4 C230901300018 EN DATA DATA-ERR DATA-MAX C230901300019 MEV MB MB MB C230901300020 29.4 0.1 C230901300021 32.3 3.5 1.2 C230901300022 35.9 16.0 3.0 C230901300023 38.9 11.0 2.0 C230901300024 ENDDATA 6 0 C230901300025 ENDSUBENT 24 0 C230901399999 SUBENT C2309014 20180815 C177C230901400001 BIB 5 14 C230901400002 REACTION (92-U-233(D,N)93-NP-234,,SIG) Spallation product. C230901400003 SAMPLE (92-U-233,ENR=0.96) C230901400004 (92-U-238,ENR=0.03) and U-234 < 1%. A few of the U233 C230901400005 targets (96% U233, 3% U238, <1% U234 were thin C230901400006 uniform deposits (~500 microg/cm2) of the hydrated C230901400007 thorium or uranium oxide electrodeposited on C230901400008 aluminum. The amount of U233 was determined by alpha C230901400009 counting of the resulting thin deposits. C230901400010 ERR-ANALYS (DATA-ERR) The limits of spallation errors are C230901400011 estimated. The quoted limits of error in the C230901400012 spallation cross sections do not include C230901400013 uncertainties in the counting efficiencies used. C230901400014 DECAY-DATA (93-NP-234,4.4D,EC) C230901400015 STATUS (TABLE) Table II, page 384. C230901400016 ENDBIB 14 0 C230901400017 NOCOMMON 0 0 C230901400018 DATA 4 7 C230901400019 EN DATA DATA-ERR DATA-MAX C230901400020 MEV MB MB MB C230901400021 9.0 1.2 C230901400022 12.1 10.5 1.6 C230901400023 14.0 10.7 1.6 C230901400024 15.4 13.2 2. C230901400025 19.6 11. 1.7 C230901400026 21.5 13.8 2.1 C230901400027 23.4 12.6 1.9 C230901400028 ENDDATA 9 0 C230901400029 ENDSUBENT 28 0 C230901499999 SUBENT C2309015 20180815 C177C230901500001 BIB 5 14 C230901500002 REACTION (92-U-233(D,2N)93-NP-233,,SIG) Spallation product. C230901500003 SAMPLE (92-U-233,ENR=0.96) C230901500004 (92-U-238,ENR=0.03) and U-234 < 1%. A few of the U233 C230901500005 targets (96% U233, 3% U238, <1% U234 were thin C230901500006 uniform deposits (~500 microg/cm2) of the hydrated C230901500007 thorium or uranium oxide electrodeposited on C230901500008 aluminum. The amount of U233 was determined by alpha C230901500009 counting of the resulting thin deposits. C230901500010 ERR-ANALYS (DATA-ERR) The limits of spallation errors are C230901500011 estimated. The quoted limits of error in the C230901500012 spallation cross sections do not include C230901500013 uncertainties in the counting efficiencies used. C230901500014 DECAY-DATA (93-NP-233,35.MIN,EC) C230901500015 STATUS (TABLE) Table II, page 384. C230901500016 ENDBIB 14 0 C230901500017 NOCOMMON 0 0 C230901500018 DATA 3 7 C230901500019 EN DATA DATA-ERR C230901500020 MEV MB MB C230901500021 9.0 0.42 0.06 C230901500022 12.1 9.4 1.9 C230901500023 14.0 10.1 1.3 C230901500024 15.4 8.7 1.2 C230901500025 19.6 3.7 1.3 C230901500026 21.5 4.36 0.59 C230901500027 23.4 5.75 0.78 C230901500028 ENDDATA 9 0 C230901500029 ENDSUBENT 28 0 C230901599999 SUBENT C2309016 20180815 C177C230901600001 BIB 5 14 C230901600002 REACTION (92-U-233(D,3N)93-NP-232,,SIG) Spallation product. C230901600003 SAMPLE (92-U-233,ENR=0.96) C230901600004 (92-U-238,ENR=0.03) and U-234 < 1%. A few of the U233 C230901600005 targets (96% U233, 3% U238, <1% U234 were thin C230901600006 uniform deposits (~500 microg/cm2) of the hydrated C230901600007 thorium or uranium oxide electrodeposited on C230901600008 aluminum. The amount of U233 was determined by alpha C230901600009 counting of the resulting thin deposits. C230901600010 ERR-ANALYS (DATA-ERR) The limits of spallation errors are C230901600011 estimated. The quoted limits of error in the C230901600012 spallation cross sections do not include C230901600013 uncertainties in the counting efficiencies used. C230901600014 DECAY-DATA (93-NP-232,13.0MIN,EC) C230901600015 STATUS (TABLE) Table II, page 384. C230901600016 ENDBIB 14 0 C230901600017 NOCOMMON 0 0 C230901600018 DATA 4 4 C230901600019 EN DATA DATA-ERR DATA-MAX C230901600020 MEV MB MB MB C230901600021 15.4 2.3 C230901600022 19.6 9.7 2. C230901600023 21.5 10.9 2.2 C230901600024 23.4 8.2 1.7 C230901600025 ENDDATA 6 0 C230901600026 ENDSUBENT 25 0 C230901699999 SUBENT C2309017 20180815 C177C230901700001 BIB 5 14 C230901700002 REACTION (92-U-233(D,X)91-PA-230,,SIG) Spallation product. C230901700003 SAMPLE (92-U-233,ENR=0.96) C230901700004 (92-U-238,ENR=0.03) and U-234 < 1%. A few of the U233 C230901700005 targets (96% U233, 3% U238, <1% U234 were thin C230901700006 uniform deposits (~500 microg/cm2) of the hydrated C230901700007 thorium or uranium oxide electrodeposited on C230901700008 aluminum. The amount of U233 was determined by alpha C230901700009 counting of the resulting thin deposits. C230901700010 ERR-ANALYS (DATA-ERR) The limits of spallation errors are C230901700011 estimated. The quoted limits of error in the C230901700012 spallation cross sections do not include C230901700013 uncertainties in the counting efficiencies used. C230901700014 DECAY-DATA (91-PA-230,17.7D,EC) C230901700015 STATUS (TABLE) Table II, page 384. C230901700016 ENDBIB 14 0 C230901700017 NOCOMMON 0 0 C230901700018 DATA 3 4 C230901700019 EN DATA DATA-ERR C230901700020 MEV MB MB C230901700021 14.0 0.08 0.03 C230901700022 15.4 0.10 0.04 C230901700023 19.6 0.91 0.36 C230901700024 23.4 1.86 0.74 C230901700025 ENDDATA 6 0 C230901700026 ENDSUBENT 25 0 C230901799999 SUBENT C2309018 20180601 C177C230901800001 BIB 6 13 C230901800002 REACTION (90-TH-232(A,F)ELEM/MASS,CUM,SIG) C230901800003 SAMPLE A few of the thorium targets were thin uniform depositsC230901800004 (~500 microg/cm2) of the hydrated thorium or uranium C230901800005 oxide electrodeposited on aluminum. The amount of C230901800006 Th232 was determined by alpha counting of the C230901800007 resulting thin deposits. C230901800008 ERR-ANALYS (DATA-ERR) The limits of fission errors are estimated. C230901800009 FLAG (1.) Isotopic-exchange difficulties which make C230901800010 ruthenium cross sections unreliable. C230901800011 CORRECTION For thorium, corrections were applied to account for C230901800012 the contribution from alpha particle-emitting C230901800013 daughters of the Th232. C230901800014 STATUS (TABLE) Table III, page 386. C230901800015 ENDBIB 13 0 C230901800016 NOCOMMON 0 0 C230901800017 DATA 8 71 C230901800018 EN-MIN EN-MAX ELEMENT MASS ISOMER DATA C230901800019 DATA-ERR FLAG C230901800020 MEV MEV NO-DIM NO-DIM NO-DIM MB C230901800021 MB NO-DIM C230901800022 15.6 19.6 38.0 89.0 0.051C230901800023 0.01 C230901800024 15.6 19.6 38.0 91.0 0.049C230901800025 0.01 C230901800026 15.6 19.6 40.0 95.0 0.11C230901800027 0.04 C230901800028 15.6 19.6 40.0 97.0 0.058C230901800029 0.02 C230901800030 15.6 19.6 48.0 115.0 0.0047C230901800031 0.003 C230901800032 15.6 19.6 48.0 115.0 0.0052C230901800033 0.004 C230901800034 15.6 19.6 56.0 140.0 0.037C230901800035 0.019 C230901800036 25.7 28.9 30.0 72.0 0.036C230901800037 0.009 C230901800038 25.7 28.9 32.0 77.0 0.083C230901800039 0.03 C230901800040 25.7 28.9 38.0 89.0 38.0C230901800041 19.0 C230901800042 25.7 28.9 38.0 91.0 66.0C230901800043 33.0 C230901800044 25.7 28.9 39.0 93.0 7.4C230901800045 3.7 C230901800046 25.7 28.9 40.0 95.0 46.0C230901800047 9.0 C230901800048 25.7 28.9 40.0 97.0 25.0C230901800049 5.0 C230901800050 25.7 28.9 42.0 99.0 28.0C230901800051 6.0 C230901800052 25.7 28.9 44.0 103.0 11.0C230901800053 2.0 1.0 C230901800054 25.7 28.9 44.0 106.0 8.6C230901800055 1.7 1.0 C230901800056 25.7 28.9 46.0 109.0 8.2C230901800057 2.1 C230901800058 25.7 28.9 46.0 112.0 8.6C230901800059 2.1 C230901800060 25.7 28.9 47.0 111.0 11.0C230901800061 2.0 C230901800062 25.7 28.9 48.0 115.0 0.0 12.0C230901800063 4.0 C230901800064 25.7 28.9 48.0 115.0 1.0 0.79C230901800065 0.2 C230901800066 25.7 28.9 48.0 115.0 13.0C230901800067 4.0 C230901800068 25.7 28.9 53.0 131.0 16.0C230901800069 4.0 C230901800070 25.7 28.9 53.0 133.0 26.0C230901800071 7.0 C230901800072 25.7 28.9 56.0 140.0 25.0C230901800073 6.0 C230901800074 34.9 37.7 30.0 72.0 0.14C230901800075 0.03 C230901800076 34.9 37.7 32.0 77.0 0.04C230901800077 0.02 C230901800078 34.9 37.7 35.0 83.0 10.0C230901800079 5.0 C230901800080 34.9 37.7 38.0 89.0 30.0C230901800081 10.0 C230901800082 34.9 37.7 38.0 91.0 34.0C230901800083 7.0 C230901800084 34.9 37.7 40.0 95.0 46.0C230901800085 9.0 C230901800086 34.9 37.7 40.0 97.0 42.0C230901800087 8.0 C230901800088 34.9 37.7 42.0 99.0 40.0C230901800089 8.0 C230901800090 34.9 37.7 44.0 103.0 15.0C230901800091 4.0 1.0 C230901800092 34.9 37.7 44.0 106.0 16.0C230901800093 3.0 1.0 C230901800094 34.9 37.7 46.0 109.0 17.0C230901800095 3.0 C230901800096 34.9 37.7 46.0 112.0 20.0C230901800097 4.0 C230901800098 34.9 37.7 47.0 111.0 27.0C230901800099 5.0 C230901800100 34.9 37.7 48.0 115.0 0.0 24.0C230901800101 5.0 C230901800102 34.9 37.7 48.0 115.0 1.0 1.4C230901800103 0.3 C230901800104 34.9 37.7 48.0 115.0 25.0C230901800105 5.0 C230901800106 34.9 37.7 53.0 131.0 22.0C230901800107 6.0 C230901800108 34.9 37.7 53.0 133.0 34.0C230901800109 14.0 C230901800110 34.9 37.7 56.0 140.0 30.0C230901800111 6.0 C230901800112 39.6 42.2 40.0 95.0 8.3C230901800113 1.7 C230901800114 39.6 42.2 40.0 97.0 7.7C230901800115 1.9 C230901800116 39.6 42.2 56.0 139.0 42.0C230901800117 12.0 C230901800118 39.6 42.2 56.0 140.0 37.0C230901800119 7.0 C230901800120 43.4 45.9 30.0 72.0 0.34C230901800121 0.07 C230901800122 43.4 45.9 32.0 77.0 0.58C230901800123 0.14 C230901800124 43.4 45.9 38.0 89.0 27.0C230901800125 6.0 C230901800126 43.4 45.9 38.0 91.0 30.0C230901800127 8.0 C230901800128 43.4 45.9 40.0 95.0 91.0C230901800129 18.0 C230901800130 43.4 45.9 40.0 97.0 73.0C230901800131 18.0 C230901800132 43.4 45.9 41.0 96.0 0.45C230901800133 0.15 C230901800134 43.4 45.9 42.0 99.0 56.0C230901800135 11.0 C230901800136 43.4 45.9 44.0 103.0 24.0C230901800137 5.0 1.0 C230901800138 43.4 45.9 44.0 105.0 23.0C230901800139 8.0 1.0 C230901800140 43.4 45.9 44.0 106.0 31.0C230901800141 6.0 1.0 C230901800142 43.4 45.9 46.0 109.0 38.0C230901800143 8.0 C230901800144 43.4 45.9 46.0 112.0 33.0C230901800145 7.0 C230901800146 43.4 45.9 47.0 111.0 63.0C230901800147 13.0 C230901800148 43.4 45.9 48.0 115.0 0.0 54.0C230901800149 27.0 C230901800150 43.4 45.9 48.0 115.0 1.0 7.8C230901800151 3.9 C230901800152 43.4 45.9 48.0 115.0 62.0C230901800153 31.0 C230901800154 43.4 45.9 56.0 140.0 30.0C230901800155 8.0 C230901800156 43.4 45.9 58.0 141.0 55.0C230901800157 11.0 C230901800158 43.4 45.9 58.0 143.0 57.0C230901800159 14.0 C230901800160 43.4 45.9 58.0 144.0 27.0C230901800161 5.0 C230901800162 43.4 45.9 60.0 147.0 11.0C230901800163 4.0 C230901800164 ENDDATA 146 0 C230901800165 ENDSUBENT 164 0 C230901899999 SUBENT C2309019 20180601 C177C230901900001 BIB 5 13 C230901900002 REACTION (90-TH-232(A,F)ELEM/MASS,,SIG) Shielded nuclide (one C230901900003 whose precursor in the b-decay chain is either stable C230901900004 or long-lived). C230901900005 SAMPLE A few of the thorium targets were thin uniform depositsC230901900006 (~500 microg/cm2) of the hydrated thorium or uranium C230901900007 oxide electrodeposited on aluminum. The amount of C230901900008 Th232 was determined by alpha counting of the C230901900009 resulting thin deposits. C230901900010 ERR-ANALYS (DATA-ERR) The limits of fission errors are estimated. C230901900011 CORRECTION For thorium, corrections were applied to account for C230901900012 the contribution from alpha particle-emitting C230901900013 daughters of the Th232. C230901900014 STATUS (TABLE) Table III, page 386. C230901900015 ENDBIB 13 0 C230901900016 NOCOMMON 0 0 C230901900017 DATA 6 12 C230901900018 EN-MIN EN-MAX ELEMENT MASS DATA DATA-ERR C230901900019 MEV MEV NO-DIM NO-DIM MB MB C230901900020 25.7 28.9 33.0 77.0 0.12 0.05C230901900021 25.7 28.9 35.0 82.0 0.034 0.01C230901900022 25.7 28.9 37.0 86.0 1.2 0.5C230901900023 25.7 28.9 55.0 136.0 2.8 0.6C230901900024 25.7 28.9 57.0 140.0 1.7 0.5C230901900025 34.9 37.7 33.0 77.0 0.37 0.11C230901900026 34.9 37.7 35.0 82.0 0.3 0.006C230901900027 34.9 37.7 37.0 86.0 0.034 0.009C230901900028 34.9 37.7 55.0 136.0 7.1 1.4C230901900029 43.4 45.9 37.0 86.0 0.099 0.025C230901900030 43.4 45.9 55.0 136.0 17.0 4.0C230901900031 43.4 45.9 57.0 140.0 3.7 1.C230901900032 ENDDATA 14 0 C230901900033 ENDSUBENT 32 0 C230901999999 SUBENT C2309020 20180606 C177C230902000001 BIB 6 12 C230902000002 REACTION (90-TH-232(A,F)ELEM/MASS,CUM,SIG) C230902000003 SAMPLE A few of the thorium targets were thin uniform depositsC230902000004 (~500 microg/cm2) of the hydrated thorium or uranium C230902000005 oxide electrodeposited on aluminum. The amount of C230902000006 Th232 was determined by alpha counting of the C230902000007 resulting thin deposits. C230902000008 ERR-ANALYS (DATA-ERR) The limits of fission errors are estimated. C230902000009 FLAG (1.) Contribution from Cd115m estimated. C230902000010 CORRECTION For thorium, corrections were applied to account for C230902000011 the contribution from alpha particle-emitting C230902000012 daughters of the Th232. C230902000013 STATUS (TABLE) Table III, page 386. C230902000014 ENDBIB 12 0 C230902000015 COMMON 1 3 C230902000016 EN-ERR C230902000017 MEV C230902000018 0.5 C230902000019 ENDCOMMON 3 0 C230902000020 DATA 7 8 C230902000021 EN ELEMENT MASS ISOMER DATA DATA-ERR C230902000022 FLAG C230902000023 MEV NO-DIM NO-DIM NO-DIM MB MB C230902000024 NO-DIM C230902000025 19.8 38.0 89.0 0.84 0.2C230902000026 C230902000027 19.8 38.0 91.0 0.96 0.32C230902000028 C230902000029 19.8 40.0 95.0 1.1 0.2C230902000030 C230902000031 19.8 40.0 97.0 1.1 0.2C230902000032 C230902000033 19.8 48.0 115.0 0.0 0.3 0.2C230902000034 C230902000035 19.8 48.0 115.0 0.32 0.31C230902000036 1.0 C230902000037 19.8 56.0 139.0 0.77 0.3C230902000038 C230902000039 19.8 56.0 140.0 0.82 0.2C230902000040 C230902000041 ENDDATA 20 0 C230902000042 ENDSUBENT 41 0 C230902099999 SUBENT C2309021 20180606 C177C230902100001 BIB 7 22 C230902100002 REACTION (90-TH-232(A,F)MASS,CHN,SIG) C230902100003 SAMPLE A few of the thorium targets were thin uniform depositsC230902100004 (~500 microg/cm2) of the hydrated thorium or uranium C230902100005 oxide electrodeposited on aluminum. The amount of C230902100006 Th232 was determined by alpha counting of the C230902100007 resulting thin deposits. C230902100008 ANALYSIS Most of the values for the chain yields are identical C230902100009 to those for the cumulative yields of the nuclide C230902100010 given in the other subentry, except that (some) cross C230902100011 sections were increased by "a small amount" to account C230902100012 for fission products of the same mass chain not C230902100013 included experimentally. C230902100014 ERR-ANALYS (DATA-ERR) The limits fission errors are estimated. C230902100015 FLAG (1.) Contribution from Cd115m estimated. C230902100016 (3.) The cross section for formation of the daughter C230902100017 was measured and found negligible. C230902100018 (4.) Isotopic-exchange difficulties which make C230902100019 ruthenium cross sections unreliable. C230902100020 CORRECTION For thorium, corrections were applied to account for C230902100021 the contribution from alpha particle-emitting C230902100022 daughters of the Th232. C230902100023 STATUS (TABLE) Table III, page 386. C230902100024 ENDBIB 22 0 C230902100025 NOCOMMON 0 0 C230902100026 DATA 6 63 C230902100027 EN-MIN EN-MAX MASS DATA DATA-ERR FLAG C230902100028 MEV MEV NO-DIM MB MB NO-DIM C230902100029 15.6 19.6 89.0 0.051 0.01 C230902100030 15.6 19.6 91.0 0.049 0.01 C230902100031 15.6 19.6 95.0 0.11 0.04 C230902100032 15.6 19.6 97.0 0.059 0.02 C230902100033 15.6 19.6 115.0 0.0052 0.004 C230902100034 15.6 19.6 140.0 0.042 0.021 C230902100035 25.7 28.9 72.0 0.038 0.01 C230902100036 25.7 28.9 77.0 0.2 0.1 C230902100037 25.7 28.9 89.0 38.0 19.0 C230902100038 25.7 28.9 91.0 66.0 33.0 3.0C230902100039 25.7 28.9 93.0 7.4 3.7 C230902100040 25.7 28.9 95.0 46.0 9.0 3.0C230902100041 25.7 28.9 97.0 25.0 5.0 C230902100042 25.7 28.9 99.0 28.0 6.0 C230902100043 25.7 28.9 103.0 11.0 0.2 4.0C230902100044 25.7 28.9 106.0 8.7 1.8 4.0C230902100045 25.7 28.9 109.0 8.2 2.1 C230902100046 25.7 28.9 111.0 11.0 2.0 C230902100047 25.7 28.9 112.0 8.8 2.2 C230902100048 25.7 28.9 115.0 13.0 4.0 C230902100049 25.7 28.9 131.0 17.0 5.0 C230902100050 25.7 28.9 133.0 32.0 9.0 C230902100051 25.7 28.9 140.0 27.0 7.0 C230902100052 34.9 37.7 72.0 0.15 0.04 C230902100053 34.9 37.7 77.0 0.41 0.13 C230902100054 34.9 37.7 83.0 10.0 5.0 C230902100055 34.9 37.7 89.0 30.0 10.0 C230902100056 34.9 37.7 91.0 35.0 8.0 C230902100057 34.9 37.7 95.0 46.0 9.0 3.0C230902100058 34.9 37.7 97.0 45.0 9.0 C230902100059 34.9 37.7 99.0 41.0 9.0 C230902100060 34.9 37.7 103.0 15.0 4.0 4.0C230902100061 34.9 37.7 106.0 17.0 4.0 4.0C230902100062 34.9 37.7 109.0 17.0 3.0 C230902100063 34.9 37.7 111.0 27.0 5.0 C230902100064 34.9 37.7 112.0 21.0 4.0 C230902100065 34.9 37.7 115.0 25.0 5.0 C230902100066 34.9 37.7 131.0 26.0 6.0 C230902100067 34.9 37.7 133.0 52.0 25.0 C230902100068 34.9 37.7 140.0 42.0 8.0 C230902100069 39.6 42.2 95.0 8.4 1.7 C230902100070 39.6 42.2 97.0 8.2 2.1 C230902100071 39.6 42.2 139.0 50.0 16.0 C230902100072 39.6 42.2 140.0 52.0 11.0 C230902100073 43.4 45.9 72.0 0.37 0.09 C230902100074 43.4 45.9 77.0 0.58 0.14 3.0C230902100075 43.4 45.9 89.0 27.0 6.0 C230902100076 43.4 45.9 91.0 30.0 8.0 3.0C230902100077 43.4 45.9 95.0 91.0 18.0 3.0C230902100078 43.4 45.9 97.0 76.0 20.0 C230902100079 43.4 45.9 99.0 56.0 11.0 C230902100080 43.4 45.9 103.0 24.0 5.0 4.0C230902100081 43.4 45.9 105.0 23.0 8.0 4.0C230902100082 43.4 45.9 106.0 32.0 6.0 4.0C230902100083 43.4 45.9 109.0 38.0 8.0 C230902100084 43.4 45.9 111.0 63.0 13.0 C230902100085 43.4 45.9 112.0 36.0 7.0 C230902100086 43.4 45.9 115.0 63.0 33.0 C230902100087 43.4 45.9 140.0 34.0 9.0 C230902100088 43.4 45.9 141.0 58.0 13.0 C230902100089 43.4 45.9 143.0 57.0 14.0 3.0C230902100090 43.4 45.9 144.0 35.0 8.0 C230902100091 43.4 45.9 147.0 12.0 5.0 C230902100092 ENDDATA 65 0 C230902100093 ENDSUBENT 92 0 C230902199999 SUBENT C2309022 20180606 C177C230902200001 BIB 7 16 C230902200002 REACTION (90-TH-232(A,F)MASS,CHN,SIG) C230902200003 SAMPLE An electroplated target. The amount of Th232 was C230902200004 determined by alpha counting of the resulting thin C230902200005 deposits. C230902200006 ANALYSIS Most of the values for the chain yields are identical C230902200007 to those for the cumulative yields of the nuclide C230902200008 given in the other subentry, except that (some) cross C230902200009 sections were increased by "a small amount" to account C230902200010 for fission products of the same mass chain not C230902200011 included experimentally. C230902200012 ERR-ANALYS (DATA-ERR) The limits of fission errors are estimated. C230902200013 FLAG (1.) Contribution from Cd115m estimated. C230902200014 CORRECTION For thorium, corrections were applied to account for C230902200015 the contribution from alpha particle-emitting C230902200016 daughters of the Th232. C230902200017 STATUS (TABLE) Table III, page 386. C230902200018 ENDBIB 16 0 C230902200019 COMMON 1 3 C230902200020 EN-ERR C230902200021 MEV C230902200022 0.5 C230902200023 ENDCOMMON 3 0 C230902200024 DATA 5 7 C230902200025 EN MASS DATA DATA-ERR FLAG C230902200026 MEV NO-DIM MB MB NO-DIM C230902200027 19.8 89.0 0.84 0.2 C230902200028 19.8 91.0 0.96 0.32 C230902200029 19.8 95.0 1.1 0.2 C230902200030 19.8 97.0 1.1 0.2 C230902200031 19.8 115.0 0.32 0.31 1.0 C230902200032 19.8 139.0 0.85 0.3 C230902200033 19.8 140.0 0.96 0.2 C230902200034 ENDDATA 9 0 C230902200035 ENDSUBENT 34 0 C230902299999 SUBENT C2309023 20180606 C177C230902300001 BIB 5 11 C230902300002 REACTION (90-TH-232(A,F)MASS,CHN,SIG) C230902300003 SAMPLE A few of the thorium targets were thin uniform depositsC230902300004 (~500 microg/cm2) of the hydrated thorium or uranium C230902300005 oxide electrodeposited on aluminum. The amount of C230902300006 Th232 was determined by alpha counting of the C230902300007 resulting thin deposits. C230902300008 ERR-ANALYS (DATA-ERR) The limits of fission errors are estimated. C230902300009 CORRECTION For thorium, corrections were applied to account for C230902300010 the contribution from alpha particle-emitting C230902300011 daughters of the Th232. C230902300012 STATUS (TABLE) Table III, page 386. C230902300013 ENDBIB 11 0 C230902300014 NOCOMMON 0 0 C230902300015 DATA 5 4 C230902300016 EN-MIN EN-MAX MASS DATA DATA-ERR C230902300017 MEV MEV NO-DIM MB MB C230902300018 25.7 28.9 77.0 0.2 0.1 C230902300019 25.7 28.9 140.0 28.0 7.0 C230902300020 34.9 37.7 77.0 0.41 0.13 C230902300021 43.4 45.9 140.0 38.0 10.0 C230902300022 ENDDATA 6 0 C230902300023 ENDSUBENT 22 0 C230902399999 SUBENT C2309024 20180606 C177C230902400001 BIB 3 9 C230902400002 REACTION (90-TH-232(A,F),,SIG) C230902400003 ERR-ANALYS (DATA-ERR) The limits of fission errors are estimated. C230902400004 STATUS (DEP,C2309004) C230902400005 (DEP,C2309005) C230902400006 (DEP,C2309006) C230902400007 (DEP,C2309007) C230902400008 (DEP,C2309008) C230902400009 (DEP,C2309009) C230902400010 (TABLE) Table III, page 386. C230902400011 ENDBIB 9 0 C230902400012 NOCOMMON 0 0 C230902400013 DATA 4 4 C230902400014 EN-MIN EN-MAX DATA DATA-ERR C230902400015 MEV MEV MB MB C230902400016 15.6 19.6 0.93 0.24 C230902400017 25.7 28.9 590.0 150.0 C230902400018 34.9 37.7 930.0 240.0 C230902400019 43.4 45.9 1660.0 410.0 C230902400020 ENDDATA 6 0 C230902400021 ENDSUBENT 20 0 C230902499999 SUBENT C2309025 20180607 C177C230902500001 BIB 4 8 C230902500002 REACTION (92-U-233(D,F)ELEM/MASS,CUM,SIG) C230902500003 SAMPLE (92-U-233,ENR=0.96) C230902500004 (92-U-238,ENR=0.03) and U-234 < 1%. An electroplated C230902500005 target. The amount of U233 was determined by alpha C230902500006 counting of the resulting thin deposits. C230902500007 ERR-ANALYS (DATA-ERR,20.,30.) The limits of erors are estimated C230902500008 to be about 20 to 30%. C230902500009 STATUS (TABLE) Table IV, page 388. C230902500010 ENDBIB 8 0 C230902500011 COMMON 1 3 C230902500012 EN-ERR C230902500013 MEV C230902500014 0.5 C230902500015 ENDCOMMON 3 0 C230902500016 DATA 6 71 C230902500017 EN ELEMENT MASS ISOMER DATA DATA-MAX C230902500018 MEV NO-DIM NO-DIM NO-DIM MB MB C230902500019 9.0 38.0 89.0 4.59 C230902500020 9.0 38.0 91.0 3.90 C230902500021 9.0 40.0 95.0 6.45 C230902500022 9.0 40.0 97.0 4.59 C230902500023 9.0 44.0 105.0 5.03 C230902500024 9.0 48.0 115.0 0.0 1.22 C230902500025 9.0 48.0 115.0 1.34 C230902500026 9.0 48.0 117.0 1.70 C230902500027 9.0 56.0 139.0 4.26 C230902500028 9.0 56.0 140.0 3.50 C230902500029 12.1 38.0 89.0 14.4 C230902500030 12.1 38.0 91.0 23.1 C230902500031 12.1 40.0 97.0 25.6 C230902500032 12.1 48.0 115.0 0.0 8.43 C230902500033 12.1 48.0 115.0 1.0 1.55C230902500034 12.1 48.0 115.0 9.98 C230902500035 12.1 48.0 117.0 12.1 C230902500036 12.1 56.0 139.0 20.4 C230902500037 12.1 56.0 140.0 17.1 C230902500038 14.0 38.0 89.0 18.9 C230902500039 14.0 38.0 91.0 18.7 C230902500040 14.0 40.0 95.0 44.8 C230902500041 14.0 40.0 97.0 39.3 C230902500042 14.0 48.0 115.0 0.0 14.7 C230902500043 14.0 48.0 115.0 1.0 1.97C230902500044 14.0 48.0 115.0 16.1 C230902500045 14.0 48.0 117.0 19.5 C230902500046 14.0 56.0 140.0 21.8 C230902500047 15.4 38.0 89.0 26.4 C230902500048 15.4 38.0 91.0 31.0 C230902500049 15.4 48.0 115.0 0.0 22.9 C230902500050 15.4 48.0 115.0 1.0 3.92C230902500051 15.4 48.0 115.0 26.8 C230902500052 15.4 48.0 117.0 21.9 C230902500053 15.4 56.0 139.0 39.3 C230902500054 15.4 56.0 140.0 29.2 C230902500055 19.6 38.0 89.0 46.5 C230902500056 19.6 38.0 91.0 36.9 C230902500057 19.6 40.0 95.0 58.5 C230902500058 19.6 40.0 97.0 49.8 C230902500059 19.6 48.0 115.0 0.0 44.0 C230902500060 19.6 48.0 115.0 1.0 5.58C230902500061 19.6 48.0 115.0 49.6 C230902500062 19.6 48.0 117.0 41.8 C230902500063 19.6 56.0 139.0 49.2 C230902500064 19.6 56.0 140.0 37.5 C230902500065 21.5 38.0 89.0 34.6 C230902500066 21.5 38.0 91.0 52.5 C230902500067 21.5 40.0 95.0 61.6 C230902500068 21.5 40.0 97.0 61.8 C230902500069 21.5 46.0 109.0 46.7 C230902500070 21.5 46.0 112.0 52.9 C230902500071 21.5 48.0 115.0 0.0 47.3 C230902500072 21.5 48.0 115.0 1.0 8.5C230902500073 21.5 48.0 115.0 55.8 C230902500074 21.5 48.0 117.0 50.0 C230902500075 21.5 56.0 139.0 46.5 C230902500076 21.5 56.0 140.0 35.5 C230902500077 23.4 38.0 89.0 42.7 C230902500078 23.4 38.0 91.0 44.3 C230902500079 23.4 40.0 95.0 54.2 C230902500080 23.4 40.0 97.0 53.5 C230902500081 23.4 48.0 115.0 0.0 63.9 C230902500082 23.4 48.0 115.0 1.0 4.8C230902500083 23.4 48.0 115.0 68.7 C230902500084 23.4 48.0 117.0 59.0 C230902500085 23.4 56.0 139.0 34.0 C230902500086 23.4 56.0 140.0 31.5 C230902500087 23.4 60.0 147.0 12.2 C230902500088 23.4 63.0 157.0 0.76 C230902500089 23.4 64.0 159.0 0.54 C230902500090 ENDDATA 73 0 C230902500091 ENDSUBENT 90 0 C230902599999 SUBENT C2309026 20180607 C177C230902600001 BIB 4 8 C230902600002 REACTION (92-U-233(D,F)MASS,CHN,SIG) C230902600003 SAMPLE (92-U-233,ENR=0.96) C230902600004 (92-U-238,ENR=0.03) and U-234 < 1%. An electroplated C230902600005 target. The amount of U233 was determined by alpha C230902600006 counting of the resulting thin deposits. C230902600007 ERR-ANALYS (DATA-ERR,20.,30.) The limits of erors are estimated C230902600008 to be about 20 to 30%. C230902600009 STATUS (TABLE) Table IV, page 388. C230902600010 ENDBIB 8 0 C230902600011 COMMON 1 3 C230902600012 EN-ERR C230902600013 MEV C230902600014 0.5 C230902600015 ENDCOMMON 3 0 C230902600016 DATA 5 71 C230902600017 EN MASS ISOMER DATA DATA-MAX C230902600018 MEV NO-DIM NO-DIM MB MB C230902600019 9.0 89.0 4.64 C230902600020 9.0 91.0 4.01 C230902600021 9.0 95.0 6.55 C230902600022 9.0 97.0 4.80 C230902600023 9.0 105.0 5.11 C230902600024 9.0 115.0 0.0 1.24 C230902600025 9.0 115.0 1.36 C230902600026 9.0 117.0 1.78 C230902600027 9.0 139.0 4.82 C230902600028 9.0 140.0 4.27 C230902600029 12.1 89.0 14.6 C230902600030 12.1 91.0 23.8 C230902600031 12.1 97.0 26.8 C230902600032 12.1 115.0 0.0 8.57 C230902600033 12.1 115.0 1.0 1.58 C230902600034 12.1 115.0 10.2 C230902600035 12.1 117.0 12.5 C230902600036 12.1 139.0 23.1 C230902600037 12.1 140.0 20.9 C230902600038 14.0 89.0 19.1 C230902600039 14.0 91.0 19.2 C230902600040 14.0 95.0 45.6 C230902600041 14.0 97.0 41.1 C230902600042 14.0 115.0 0.0 15.0 C230902600043 14.0 115.0 1.0 2.0 C230902600044 14.0 115.0 17.0 C230902600045 14.0 117.0 20.4 C230902600046 14.0 140.0 26.6 C230902600047 15.4 89.0 26.7 C230902600048 15.4 91.0 32.0 C230902600049 15.4 115.0 0.0 23.4 C230902600050 15.4 115.0 1.0 4.0 C230902600051 15.4 115.0 27.4 C230902600052 15.4 117.0 23.2 C230902600053 15.4 139.0 46.2 C230902600054 15.4 140.0 41.7 C230902600055 19.6 89.0 48.2 C230902600056 19.6 91.0 38.0 C230902600057 19.6 95.0 59.7 C230902600058 19.6 97.0 52.4 C230902600059 19.6 115.0 0.0 45.0 C230902600060 19.6 115.0 1.0 5.70 C230902600061 19.6 115.0 50.7 C230902600062 19.6 117.0 44.2 C230902600063 19.6 139.0 57.9 C230902600064 19.6 140.0 53.6 C230902600065 21.5 89.0 35.1 C230902600066 21.5 91.0 54.6 C230902600067 21.5 95.0 63.0 C230902600068 21.5 97.0 66.0 C230902600069 21.5 109.0 47.5 C230902600070 21.5 112.0 56.9 C230902600071 21.5 115.0 0.0 48.6 C230902600072 21.5 115.0 1.0 8.7 C230902600073 21.5 115.0 57.3 C230902600074 21.5 117.0 53.8 C230902600075 21.5 139.0 58.1 C230902600076 21.5 140.0 53.0 C230902600077 23.4 89.0 43.3 C230902600078 23.4 91.0 46.2 C230902600079 23.4 95.0 55.5 C230902600080 23.4 97.0 57.2 C230902600081 23.4 115.0 0.0 65.7 C230902600082 23.4 115.0 1.0 4.9 C230902600083 23.4 115.0 70.6 C230902600084 23.4 117.0 63.5 C230902600085 23.4 139.0 45.3 C230902600086 23.4 140.0 47.0 C230902600087 23.4 147.0 13.3 C230902600088 23.4 157.0 1.03 C230902600089 23.4 159.0 0.70 C230902600090 ENDDATA 73 0 C230902600091 ENDSUBENT 90 0 C230902699999 SUBENT C2309027 20180607 C177C230902700001 BIB 4 9 C230902700002 REACTION (92-U-233(D,F),,SIG) C230902700003 SAMPLE (92-U-233,ENR=0.96) C230902700004 (92-U-238,ENR=0.03) and U-234 < 1%. An electroplated C230902700005 target. The amount of U233 was determined by alpha C230902700006 counting of the resulting thin deposits. C230902700007 ERR-ANALYS (DATA-ERR) The limits of fission errors are estimated. C230902700008 STATUS (DEP,C2309012) C230902700009 (DEP,C2309013) C230902700010 (TABLE) Table IV, page 388. C230902700011 ENDBIB 9 0 C230902700012 NOCOMMON 0 0 C230902700013 DATA 3 7 C230902700014 EN DATA DATA-ERR C230902700015 MEV MB MB C230902700016 9.0 125.0 34.0 C230902700017 12.1 605.0 163.0 C230902700018 14.0 857.0 231.0 C230902700019 15.4 1093.0 295.0 C230902700020 19.6 1502.0 406.0 C230902700021 21.5 1687.0 456.0 C230902700022 23.4 1861.0 503.0 C230902700023 ENDDATA 9 0 C230902700024 ENDSUBENT 23 0 C230902799999 ENDENTRY 27 0 C230999999999