ENTRY C2309 20230112 C227C2309000 1 SUBENT C2309001 20230112 C227C2309001 1 BIB 9 32 C2309001 2 TITLE Spallation-fission competition in heavy-element C2309001 3 reactions: Th232+He4 and U233+d C2309001 4 AUTHOR (B.M.Foreman Jr,W.M.Gibson,R.A.Glass,G.T.Seaborg) C2309001 5 REFERENCE (J,PR,116,382,1959) C2309001 6 #doi:10.1103/physrev.116.382 C2309001 7 (R,UCRL-3493,1956) Preliminary U233 report data. C2309001 8 REL-REF (O,C2882001,W.M.Gibson+,R,UCRL-3493,1956) Related C2309001 9 Pu239 and Np237 data from Berkeley report. C2309001 10 INSTITUTE (1USABRK,1USAUCX) C2309001 11 FACILITY (CYCLO,1USABRK) Berkeley 60-inch cyclotron. C2309001 12 DETECTOR (PROPC) C2309001 13 METHOD (CHSEP,ACTIV) For the thorium foil bombardments the C2309001 14 large amounts of activity produced allowed separate C2309001 15 aliquots of the dissolved target to Be used for the C2309001 16 various fractions analyzed. For the thorium C2309001 17 bombardments the protactinium fraction was purified C2309001 18 by extraction with diisopropyl ketone (dipk) and C2309001 19 elution on an anion-exchange column. The uranium C2309001 20 fraction was purified by an anion-exchange-column C2309001 21 elution. For the U233 bombardments the chemical C2309001 22 separation of the neptunium fraction was described by C2309001 23 vandenbosch. The protactinium fraction was separated C2309001 24 from the neptunium by carrying neptunium (iv) C2309001 25 fluoride on laf3. the counting rates of C2309001 26 alpha-particle-emitting spallation products were C2309001 27 measured by use of a multichannel alpha-pulse-height C2309001 28 analyzer. The counting rates of spallation products C2309001 29 which decay by orbital electron capture were C2309001 30 determined with a methane-flow windowless C2309001 31 proportional counter. C2309001 32 HISTORY (20180601C) BP C2309001 33 (20230112A) BP: Added REL-REF and Berkeley report. C2309001 34 ENDBIB 32 0 C2309001 35 COMMON 1 3 C2309001 36 EN-ERR C2309001 37 MEV C2309001 38 0.5 C2309001 39 ENDCOMMON 3 0 C2309001 40 ENDSUBENT 39 0 C230900199999 SUBENT C2309002 20180815 C177C2309 2 1 BIB 6 15 C2309 2 2 REACTION (90-TH-232(A,4N)92-U-232,,SIG) Spallation product. C2309 2 3 SAMPLE A few of the thorium targets were thin uniform depositsC2309 2 4 (~500 microg/cm2) of the hydrated thorium or uranium C2309 2 5 oxide electrodeposited on aluminum. The amount of C2309 2 6 Th232 was determined by alpha counting of the C2309 2 7 resulting thin deposits. C2309 2 8 ERR-ANALYS (DATA-ERR) The limits of spallation errors are C2309 2 9 estimated. The quoted limits of error in the C2309 2 10 spallation cross sections do not include C2309 2 11 uncertainties in the counting efficiencies used. C2309 2 12 DECAY-DATA (92-U-232,70.0YR,A) C2309 2 13 CORRECTION For thorium, corrections were applied to account for C2309 2 14 the contribution from alpha particle-emitting C2309 2 15 daughters of the Th232. C2309 2 16 STATUS (TABLE) Table I, page 384. C2309 2 17 ENDBIB 15 0 C2309 2 18 NOCOMMON 0 0 C2309 2 19 DATA 5 15 C2309 2 20 EN-MIN EN-MAX DATA DATA-ERR DATA-MAX C2309 2 21 MEV MEV MB MB MB C2309 2 22 25.7 28.9 0.008 C2309 2 23 29.9 31.8 0.11 0.06 C2309 2 24 30.6 33.4 1. 0.1 C2309 2 25 32.0 33.7 0.12 0.01 C2309 2 26 34.8 36.9 17.9 1.8 C2309 2 27 34.9 37.7 15.6 1.6 C2309 2 28 34.9 37.7 19. 1.9 C2309 2 29 35.8 37.8 17.5 1.8 C2309 2 30 39.0 41.6 54.5 5.5 C2309 2 31 39.3 41.0 54.7 5.5 C2309 2 32 43.4 45.9 3.7 1. C2309 2 33 43.4 45.9 34.7 3.7 C2309 2 34 43.4 45.9 33.4 3.3 C2309 2 35 43.4 45.9 100.0 C2309 2 36 43.8 45.4 31.6 3.2 C2309 2 37 ENDDATA 17 0 C2309 2 38 ENDSUBENT 37 0 C2309 299999 SUBENT C2309003 20180815 C177C2309 3 1 BIB 6 15 C2309 3 2 REACTION (90-TH-232(A,5N)92-U-231,,SIG) Spallation product. C2309 3 3 SAMPLE A few of the thorium targets were thin uniform depositsC2309 3 4 (~500 microg/cm2) of the hydrated thorium or uranium C2309 3 5 oxide electrodeposited on aluminum. The amount of C2309 3 6 Th232 was determined by alpha counting of the C2309 3 7 resulting thin deposits. C2309 3 8 ERR-ANALYS (DATA-ERR) The limits of spallation errors are C2309 3 9 estimated. The quoted limits of error in the C2309 3 10 spallation cross sections do not include C2309 3 11 uncertainties in the counting efficiencies used. C2309 3 12 DECAY-DATA (92-U-231,4.3D,A) C2309 3 13 CORRECTION For thorium, corrections were applied to account for C2309 3 14 the contribution from alpha particle-emitting C2309 3 15 daughters of the Th232. C2309 3 16 STATUS (TABLE) Table I, page 384. C2309 3 17 ENDBIB 15 0 C2309 3 18 NOCOMMON 0 0 C2309 3 19 DATA 4 1 C2309 3 20 EN-MIN EN-MAX DATA DATA-ERR C2309 3 21 MEV MEV MB MB C2309 3 22 43.4 45.9 3.7 1.0 C2309 3 23 ENDDATA 3 0 C2309 3 24 ENDSUBENT 23 0 C2309 399999 SUBENT C2309004 20180815 C177C2309 4 1 BIB 6 15 C2309 4 2 REACTION (90-TH-232(A,P)91-PA-235,,SIG) Spallation product. C2309 4 3 SAMPLE A few of the thorium targets were thin uniform depositsC2309 4 4 (~500 microg/cm2) of the hydrated thorium or uranium C2309 4 5 oxide electrodeposited on aluminum. The amount of C2309 4 6 Th232 was determined by alpha counting of the C2309 4 7 resulting thin deposits. C2309 4 8 ERR-ANALYS (DATA-ERR) The limits of spallation errors are C2309 4 9 estimated. The quoted limits of error in the C2309 4 10 spallation cross sections do not include C2309 4 11 uncertainties in the counting efficiencies used. C2309 4 12 DECAY-DATA (91-PA-235,23.7MIN,B-) C2309 4 13 CORRECTION For thorium, corrections were applied to account for C2309 4 14 the contribution from alpha particle-emitting C2309 4 15 daughters of the Th232. C2309 4 16 STATUS (TABLE) Table I, page 384. C2309 4 17 ENDBIB 15 0 C2309 4 18 NOCOMMON 0 0 C2309 4 19 DATA 5 9 C2309 4 20 EN-MIN EN-MAX DATA DATA-ERR DATA-MAX C2309 4 21 MEV MEV MB MB MB C2309 4 22 21.6 23.9 0.07 C2309 4 23 25.7 28.1 1.14 0.4 C2309 4 24 27.6 29.9 0.64 0.21 C2309 4 25 29.9 31.8 3.4 0.6 C2309 4 26 32.0 33.7 3.3 1.2 C2309 4 27 34.8 36.9 2.9 0.6 C2309 4 28 35.8 37.8 5.4 2.0 C2309 4 29 39.3 41.0 3.0 1.5 C2309 4 30 43.8 45.4 1.7 C2309 4 31 ENDDATA 11 0 C2309 4 32 ENDSUBENT 31 0 C2309 499999 SUBENT C2309005 20180815 C177C2309 5 1 BIB 6 15 C2309 5 2 REACTION (90-TH-232(A,X)91-PA-234-G,CUM,SIG) Spallation product.C2309 5 3 SAMPLE A few of the thorium targets were thin uniform depositsC2309 5 4 (~500 microg/cm2) of the hydrated thorium or uranium C2309 5 5 oxide electrodeposited on aluminum. The amount of C2309 5 6 Th232 was determined by alpha counting of the C2309 5 7 resulting thin deposits. C2309 5 8 ERR-ANALYS (DATA-ERR) The limits of spallation errors are C2309 5 9 estimated. The quoted limits of error in the C2309 5 10 spallation cross sections do not include C2309 5 11 uncertainties in the counting efficiencies used. C2309 5 12 DECAY-DATA (91-PA-234-G,6.7HR,B-) C2309 5 13 CORRECTION For thorium, corrections were applied to account for C2309 5 14 the contribution from alpha particle-emitting C2309 5 15 daughters of the Th232. C2309 5 16 STATUS (TABLE) Table I, page 384. C2309 5 17 ENDBIB 15 0 C2309 5 18 NOCOMMON 0 0 C2309 5 19 DATA 4 10 C2309 5 20 EN-MIN EN-MAX DATA DATA-ERR C2309 5 21 MEV MEV MB MB C2309 5 22 25.7 28.1 0.61 0.2 C2309 5 23 27.6 29.9 0.41 0.04 C2309 5 24 29.9 31.8 5.2 0.5 C2309 5 25 32.0 33.7 6.4 0.6 C2309 5 26 34.8 36.9 16.0 2.0 C2309 5 27 35.8 37.8 21.0 2.0 C2309 5 28 39.0 41.6 21.0 2.0 C2309 5 29 39.3 41.0 22.0 2.0 C2309 5 30 43.4 45.9 18.0 2.0 C2309 5 31 43.8 45.4 19.0 4.0 C2309 5 32 ENDDATA 12 0 C2309 5 33 ENDSUBENT 32 0 C2309 599999 SUBENT C2309006 20180815 C177C2309 6 1 BIB 6 15 C2309 6 2 REACTION (90-TH-232(A,X)91-PA-233,CUM,SIG) Spallation product. C2309 6 3 SAMPLE A few of the thorium targets were thin uniform depositsC2309 6 4 (~500 microg/cm2) of the hydrated thorium or uranium C2309 6 5 oxide electrodeposited on aluminum. The amount of C2309 6 6 Th232 was determined by alpha counting of the C2309 6 7 resulting thin deposits. C2309 6 8 ERR-ANALYS (DATA-ERR) The limits of spallation errors are C2309 6 9 estimated. The quoted limits of error in the C2309 6 10 spallation cross sections do not include C2309 6 11 uncertainties in the counting efficiencies used. C2309 6 12 DECAY-DATA (91-PA-233,27.0D,B-) C2309 6 13 CORRECTION For thorium, corrections were applied to account for C2309 6 14 the contribution from alpha particle-emitting C2309 6 15 daughters of the Th232. C2309 6 16 STATUS (TABLE) Table I, page 384. C2309 6 17 ENDBIB 15 0 C2309 6 18 NOCOMMON 0 0 C2309 6 19 DATA 4 14 C2309 6 20 EN-MIN EN-MAX DATA DATA-ERR C2309 6 21 MEV MEV MB MB C2309 6 22 15.0 18.0 0.21 0.02 C2309 6 23 19.9 22.4 0.21 0.03 C2309 6 24 21.6 23.9 0.41 0.05 C2309 6 25 23.6 25.9 0.31 0.05 C2309 6 26 25.7 28.1 3.3 0.4 C2309 6 27 27.6 29.9 2.4 0.3 C2309 6 28 29.9 31.8 8.5 0.9 C2309 6 29 32.0 33.7 10.0 1.0 C2309 6 30 34.8 36.9 14.0 2.0 C2309 6 31 35.8 37.8 17.0 2.0 C2309 6 32 39.0 41.6 18.0 2.0 C2309 6 33 39.3 41.0 21.0 2.0 C2309 6 34 43.4 45.9 22.0 3.0 C2309 6 35 43.8 45.4 24.0 5.0 C2309 6 36 ENDDATA 16 0 C2309 6 37 ENDSUBENT 36 0 C2309 699999 SUBENT C2309007 20180815 C177C2309 7 1 BIB 6 15 C2309 7 2 REACTION (90-TH-232(A,X)91-PA-232,,SIG) Spallation product. C2309 7 3 SAMPLE A few of the thorium targets were thin uniform depositsC2309 7 4 (~500 microg/cm2) of the hydrated thorium or uranium C2309 7 5 oxide electrodeposited on aluminum. The amount of C2309 7 6 Th232 was determined by alpha counting of the C2309 7 7 resulting thin deposits. C2309 7 8 ERR-ANALYS (DATA-ERR) The limits of spallation errors are C2309 7 9 estimated. The quoted limits of error in the C2309 7 10 spallation cross sections do not include C2309 7 11 uncertainties in the counting efficiencies used. C2309 7 12 DECAY-DATA (91-PA-232,1.31D,B-) C2309 7 13 CORRECTION For thorium, corrections were applied to account for C2309 7 14 the contribution from alpha particle-emitting C2309 7 15 daughters of the Th232. C2309 7 16 STATUS (TABLE) Table I, page 384. C2309 7 17 ENDBIB 15 0 C2309 7 18 NOCOMMON 0 0 C2309 7 19 DATA 4 11 C2309 7 20 EN-MIN EN-MAX DATA DATA-ERR C2309 7 21 MEV MEV MB MB C2309 7 22 15.0 18.0 0.11 0.002 C2309 7 23 19.9 22.4 0.016 0.03 C2309 7 24 21.6 23.9 0.02 0.006 C2309 7 25 27.6 29.9 0.08 0.02 C2309 7 26 29.9 31.8 0.34 0.1 C2309 7 27 32.0 33.7 0.25 0.05 C2309 7 28 34.8 36.9 0.93 0.2 C2309 7 29 35.8 37.8 1.8 0.4 C2309 7 30 39.3 41.0 2.3 0.4 C2309 7 31 43.4 45.9 5.2 1.1 C2309 7 32 43.8 45.4 4.1 1.0 C2309 7 33 ENDDATA 13 0 C2309 7 34 ENDSUBENT 33 0 C2309 799999 SUBENT C2309008 20180815 C177C2309 8 1 BIB 6 15 C2309 8 2 REACTION (90-TH-232(A,2P)90-TH-234,,SIG) Spallation product. C2309 8 3 SAMPLE A few of the thorium targets were thin uniform depositsC2309 8 4 (~500 microg/cm2) of the hydrated thorium or uranium C2309 8 5 oxide electrodeposited on aluminum. The amount of C2309 8 6 Th232 was determined by alpha counting of the C2309 8 7 resulting thin deposits. C2309 8 8 ERR-ANALYS (DATA-ERR) The limits of spallation errors are C2309 8 9 estimated. The quoted limits of error in the C2309 8 10 spallation cross sections do not include C2309 8 11 uncertainties in the counting efficiencies used. C2309 8 12 DECAY-DATA (90-TH-234,24.1D,B-) C2309 8 13 CORRECTION For thorium, corrections were applied to account for C2309 8 14 the contribution from alpha particle-emitting C2309 8 15 daughters of the Th232. C2309 8 16 STATUS (TABLE) Table I, page 384. C2309 8 17 ENDBIB 15 0 C2309 8 18 NOCOMMON 0 0 C2309 8 19 DATA 5 6 C2309 8 20 EN-MIN EN-MAX DATA DATA-ERR DATA-MAX C2309 8 21 MEV MEV MB MB MB C2309 8 22 25.7 28.1 0.16 0.08 C2309 8 23 29.9 31.8 0.055 0.028 C2309 8 24 30.6 33.4 0.01 C2309 8 25 32.0 33.7 0.08 C2309 8 26 39.0 41.6 6.0 C2309 8 27 43.4 45.9 0.07 C2309 8 28 ENDDATA 8 0 C2309 8 29 ENDSUBENT 28 0 C2309 899999 SUBENT C2309009 20180815 C177C2309 9 1 BIB 6 15 C2309 9 2 REACTION (90-TH-232(A,X)90-TH-233,CUM,SIG) Spallation product. C2309 9 3 SAMPLE A few of the thorium targets were thin uniform depositsC2309 9 4 (~500 microg/cm2) of the hydrated thorium or uranium C2309 9 5 oxide electrodeposited on aluminum. The amount of C2309 9 6 Th232 was determined by alpha counting of the C2309 9 7 resulting thin deposits. C2309 9 8 ERR-ANALYS (DATA-ERR) The limits of spallation errors are C2309 9 9 estimated. The quoted limits of error in the C2309 9 10 spallation cross sections do not include C2309 9 11 uncertainties in the counting efficiencies used. C2309 9 12 DECAY-DATA (90-TH-233,23.3MIN,B-) C2309 9 13 CORRECTION For thorium, corrections were applied to account for C2309 9 14 the contribution from alpha particle-emitting C2309 9 15 daughters of the Th232. C2309 9 16 STATUS (TABLE) Table I, page 384. C2309 9 17 ENDBIB 15 0 C2309 9 18 NOCOMMON 0 0 C2309 9 19 DATA 5 9 C2309 9 20 EN-MIN EN-MAX DATA DATA-ERR DATA-MAX C2309 9 21 MEV MEV MB MB MB C2309 9 22 19.9 22.4 0.11 0.06 C2309 9 23 21.6 23.9 0.14 C2309 9 24 25.7 28.1 0.54 0.27 C2309 9 25 29.9 31.8 0.62 0.31 C2309 9 26 32.0 33.7 2.9 1.1 C2309 9 27 34.8 36.9 0.36 0.19 C2309 9 28 35.8 37.8 1.9 1.4 C2309 9 29 39.3 41.0 2.0 0.7 C2309 9 30 43.8 45.4 4.2 1.5 C2309 9 31 ENDDATA 11 0 C2309 9 32 ENDSUBENT 31 0 C2309 999999 SUBENT C2309010 20180815 C177C2309 10 1 BIB 6 15 C2309 10 2 REACTION (90-TH-232(A,X)90-TH-231,CUM,SIG) Spallation product. C2309 10 3 SAMPLE A few of the thorium targets were thin uniform depositsC2309 10 4 (~500 microg/cm2) of the hydrated thorium or uranium C2309 10 5 oxide electrodeposited on aluminum. The amount of C2309 10 6 Th232 was determined by alpha counting of the C2309 10 7 resulting thin deposits. C2309 10 8 ERR-ANALYS (DATA-ERR) The limits of spallation errors are C2309 10 9 estimated. The quoted limits of error in the C2309 10 10 spallation cross sections do not include C2309 10 11 uncertainties in the counting efficiencies used. C2309 10 12 DECAY-DATA (90-TH-231,25.6HR,B-) C2309 10 13 CORRECTION For thorium, corrections were applied to account for C2309 10 14 the contribution from alpha particle-emitting C2309 10 15 daughters of the Th232. C2309 10 16 STATUS (TABLE) Table I, page 384. C2309 10 17 ENDBIB 15 0 C2309 10 18 NOCOMMON 0 0 C2309 10 19 DATA 5 17 C2309 10 20 EN-MIN EN-MAX DATA DATA-ERR DATA-MAX C2309 10 21 MEV MEV MB MB MB C2309 10 22 15.0 18.0 3.6 1.2 C2309 10 23 19.9 22.4 0.93 0.4 C2309 10 24 21.6 23.9 0.14 C2309 10 25 25.7 28.1 0.84 0.28 C2309 10 26 27.6 29.9 3.6 1.2 C2309 10 27 29.9 31.8 2.3 0.8 C2309 10 28 30.6 33.4 1.5 0.6 C2309 10 29 34.8 36.9 16.0 2.0 C2309 10 30 34.9 37.7 20.0 4.0 C2309 10 31 34.9 37.7 12.0 3.0 C2309 10 32 35.8 37.8 28.0 7.0 C2309 10 33 39.0 41.6 37.0 19.0 C2309 10 34 39.3 41.0 15.0 5.0 C2309 10 35 39.6 42.2 31.0 6.0 C2309 10 36 43.4 45.9 42.0 8.0 C2309 10 37 43.4 45.9 49.0 14.0 C2309 10 38 43.8 45.4 35.0 9.0 C2309 10 39 ENDDATA 19 0 C2309 10 40 ENDSUBENT 39 0 C2309 1099999 SUBENT C2309011 20180815 C177C2309 11 1 BIB 6 13 C2309 11 2 REACTION (90-TH-232(A,4N)92-U-232,,SIG) Spallation product. C2309 11 3 SAMPLE An electroplated target. The amount of C2309 11 4 Th232 was determined by alpha counting of the C2309 11 5 resulting thin deposits. C2309 11 6 ERR-ANALYS (DATA-ERR) The limits of spallation errors are C2309 11 7 estimated. The quoted limits of error in the C2309 11 8 spallation cross sections do not include C2309 11 9 uncertainties in the counting efficiencies used. C2309 11 10 DECAY-DATA (92-U-232,70.0YR,A) C2309 11 11 CORRECTION For thorium, corrections were applied to account for C2309 11 12 the contribution from alpha particle-emitting C2309 11 13 daughters of the Th232. C2309 11 14 STATUS (TABLE) Table I, page 384. C2309 11 15 ENDBIB 13 0 C2309 11 16 NOCOMMON 0 0 C2309 11 17 DATA 4 2 C2309 11 18 EN DATA DATA-ERR DATA-MAX C2309 11 19 MEV MB MB MB C2309 11 20 32.3 30.0 C2309 11 21 38.9 27.9 2.8 C2309 11 22 ENDDATA 4 0 C2309 11 23 ENDSUBENT 22 0 C2309 1199999 SUBENT C2309012 20180815 C177C2309 12 1 BIB 5 9 C2309 12 2 REACTION (90-TH-232(A,2P)90-TH-234,,SIG) Spallation product. C2309 12 3 SAMPLE An electroplated target. The amount of C2309 12 4 Th232 was determined by alpha counting of the C2309 12 5 resulting thin deposits. C2309 12 6 DECAY-DATA (90-TH-234,24.1D,B-) C2309 12 7 CORRECTION For thorium, corrections were applied to account for C2309 12 8 the contribution from alpha particle-emitting C2309 12 9 daughters of the Th232. C2309 12 10 STATUS (TABLE) Table I, page 384. C2309 12 11 ENDBIB 9 0 C2309 12 12 NOCOMMON 0 0 C2309 12 13 DATA 2 2 C2309 12 14 EN DATA-MAX C2309 12 15 MEV MB C2309 12 16 26.5 2.1 C2309 12 17 35.9 0.2 C2309 12 18 ENDDATA 4 0 C2309 12 19 ENDSUBENT 18 0 C2309 1299999 SUBENT C2309013 20180815 C177C2309 13 1 BIB 6 13 C2309 13 2 REACTION (90-TH-232(A,X)90-TH-231,CUM,SIG) Spallation product C2309 13 3 SAMPLE An electroplated target. The amount of C2309 13 4 Th232 was determined by alpha counting of the C2309 13 5 resulting thin deposits. C2309 13 6 ERR-ANALYS (DATA-ERR) The limits of spallation errors are C2309 13 7 estimated. The quoted limits of error in the C2309 13 8 spallation cross sections do not include C2309 13 9 uncertainties in the counting efficiencies used. C2309 13 10 DECAY-DATA (90-TH-231,25.6HR,B-) C2309 13 11 CORRECTION For thorium, corrections were applied to account for C2309 13 12 the contribution from alpha particle-emitting C2309 13 13 daughters of the Th232. C2309 13 14 STATUS (TABLE) Table I, page 384. C2309 13 15 ENDBIB 13 0 C2309 13 16 NOCOMMON 0 0 C2309 13 17 DATA 4 4 C2309 13 18 EN DATA DATA-ERR DATA-MAX C2309 13 19 MEV MB MB MB C2309 13 20 29.4 0.1 C2309 13 21 32.3 3.5 1.2 C2309 13 22 35.9 16.0 3.0 C2309 13 23 38.9 11.0 2.0 C2309 13 24 ENDDATA 6 0 C2309 13 25 ENDSUBENT 24 0 C2309 1399999 SUBENT C2309014 20180815 C177C2309 14 1 BIB 5 14 C2309 14 2 REACTION (92-U-233(D,N)93-NP-234,,SIG) Spallation product. C2309 14 3 SAMPLE (92-U-233,ENR=0.96) C2309 14 4 (92-U-238,ENR=0.03) and U-234 < 1%. A few of the U233 C2309 14 5 targets (96% U233, 3% U238, <1% U234 were thin C2309 14 6 uniform deposits (~500 microg/cm2) of the hydrated C2309 14 7 thorium or uranium oxide electrodeposited on C2309 14 8 aluminum. The amount of U233 was determined by alpha C2309 14 9 counting of the resulting thin deposits. C2309 14 10 ERR-ANALYS (DATA-ERR) The limits of spallation errors are C2309 14 11 estimated. The quoted limits of error in the C2309 14 12 spallation cross sections do not include C2309 14 13 uncertainties in the counting efficiencies used. C2309 14 14 DECAY-DATA (93-NP-234,4.4D,EC) C2309 14 15 STATUS (TABLE) Table II, page 384. C2309 14 16 ENDBIB 14 0 C2309 14 17 NOCOMMON 0 0 C2309 14 18 DATA 4 7 C2309 14 19 EN DATA DATA-ERR DATA-MAX C2309 14 20 MEV MB MB MB C2309 14 21 9.0 1.2 C2309 14 22 12.1 10.5 1.6 C2309 14 23 14.0 10.7 1.6 C2309 14 24 15.4 13.2 2. C2309 14 25 19.6 11. 1.7 C2309 14 26 21.5 13.8 2.1 C2309 14 27 23.4 12.6 1.9 C2309 14 28 ENDDATA 9 0 C2309 14 29 ENDSUBENT 28 0 C2309 1499999 SUBENT C2309015 20180815 C177C2309 15 1 BIB 5 14 C2309 15 2 REACTION (92-U-233(D,2N)93-NP-233,,SIG) Spallation product. C2309 15 3 SAMPLE (92-U-233,ENR=0.96) C2309 15 4 (92-U-238,ENR=0.03) and U-234 < 1%. A few of the U233 C2309 15 5 targets (96% U233, 3% U238, <1% U234 were thin C2309 15 6 uniform deposits (~500 microg/cm2) of the hydrated C2309 15 7 thorium or uranium oxide electrodeposited on C2309 15 8 aluminum. The amount of U233 was determined by alpha C2309 15 9 counting of the resulting thin deposits. C2309 15 10 ERR-ANALYS (DATA-ERR) The limits of spallation errors are C2309 15 11 estimated. The quoted limits of error in the C2309 15 12 spallation cross sections do not include C2309 15 13 uncertainties in the counting efficiencies used. C2309 15 14 DECAY-DATA (93-NP-233,35.MIN,EC) C2309 15 15 STATUS (TABLE) Table II, page 384. C2309 15 16 ENDBIB 14 0 C2309 15 17 NOCOMMON 0 0 C2309 15 18 DATA 3 7 C2309 15 19 EN DATA DATA-ERR C2309 15 20 MEV MB MB C2309 15 21 9.0 0.42 0.06 C2309 15 22 12.1 9.4 1.9 C2309 15 23 14.0 10.1 1.3 C2309 15 24 15.4 8.7 1.2 C2309 15 25 19.6 3.7 1.3 C2309 15 26 21.5 4.36 0.59 C2309 15 27 23.4 5.75 0.78 C2309 15 28 ENDDATA 9 0 C2309 15 29 ENDSUBENT 28 0 C2309 1599999 SUBENT C2309016 20180815 C177C2309 16 1 BIB 5 14 C2309 16 2 REACTION (92-U-233(D,3N)93-NP-232,,SIG) Spallation product. C2309 16 3 SAMPLE (92-U-233,ENR=0.96) C2309 16 4 (92-U-238,ENR=0.03) and U-234 < 1%. A few of the U233 C2309 16 5 targets (96% U233, 3% U238, <1% U234 were thin C2309 16 6 uniform deposits (~500 microg/cm2) of the hydrated C2309 16 7 thorium or uranium oxide electrodeposited on C2309 16 8 aluminum. The amount of U233 was determined by alpha C2309 16 9 counting of the resulting thin deposits. C2309 16 10 ERR-ANALYS (DATA-ERR) The limits of spallation errors are C2309 16 11 estimated. The quoted limits of error in the C2309 16 12 spallation cross sections do not include C2309 16 13 uncertainties in the counting efficiencies used. C2309 16 14 DECAY-DATA (93-NP-232,13.0MIN,EC) C2309 16 15 STATUS (TABLE) Table II, page 384. C2309 16 16 ENDBIB 14 0 C2309 16 17 NOCOMMON 0 0 C2309 16 18 DATA 4 4 C2309 16 19 EN DATA DATA-ERR DATA-MAX C2309 16 20 MEV MB MB MB C2309 16 21 15.4 2.3 C2309 16 22 19.6 9.7 2. C2309 16 23 21.5 10.9 2.2 C2309 16 24 23.4 8.2 1.7 C2309 16 25 ENDDATA 6 0 C2309 16 26 ENDSUBENT 25 0 C2309 1699999 SUBENT C2309017 20180815 C177C2309 17 1 BIB 5 14 C2309 17 2 REACTION (92-U-233(D,X)91-PA-230,,SIG) Spallation product. C2309 17 3 SAMPLE (92-U-233,ENR=0.96) C2309 17 4 (92-U-238,ENR=0.03) and U-234 < 1%. A few of the U233 C2309 17 5 targets (96% U233, 3% U238, <1% U234 were thin C2309 17 6 uniform deposits (~500 microg/cm2) of the hydrated C2309 17 7 thorium or uranium oxide electrodeposited on C2309 17 8 aluminum. The amount of U233 was determined by alpha C2309 17 9 counting of the resulting thin deposits. C2309 17 10 ERR-ANALYS (DATA-ERR) The limits of spallation errors are C2309 17 11 estimated. The quoted limits of error in the C2309 17 12 spallation cross sections do not include C2309 17 13 uncertainties in the counting efficiencies used. C2309 17 14 DECAY-DATA (91-PA-230,17.7D,EC) C2309 17 15 STATUS (TABLE) Table II, page 384. C2309 17 16 ENDBIB 14 0 C2309 17 17 NOCOMMON 0 0 C2309 17 18 DATA 3 4 C2309 17 19 EN DATA DATA-ERR C2309 17 20 MEV MB MB C2309 17 21 14.0 0.08 0.03 C2309 17 22 15.4 0.10 0.04 C2309 17 23 19.6 0.91 0.36 C2309 17 24 23.4 1.86 0.74 C2309 17 25 ENDDATA 6 0 C2309 17 26 ENDSUBENT 25 0 C2309 1799999 SUBENT C2309018 20180601 C177C2309 18 1 BIB 6 13 C2309 18 2 REACTION (90-TH-232(A,F)ELEM/MASS,CUM,SIG) C2309 18 3 SAMPLE A few of the thorium targets were thin uniform depositsC2309 18 4 (~500 microg/cm2) of the hydrated thorium or uranium C2309 18 5 oxide electrodeposited on aluminum. The amount of C2309 18 6 Th232 was determined by alpha counting of the C2309 18 7 resulting thin deposits. C2309 18 8 ERR-ANALYS (DATA-ERR) The limits of fission errors are estimated. C2309 18 9 FLAG (1.) Isotopic-exchange difficulties which make C2309 18 10 ruthenium cross sections unreliable. C2309 18 11 CORRECTION For thorium, corrections were applied to account for C2309 18 12 the contribution from alpha particle-emitting C2309 18 13 daughters of the Th232. C2309 18 14 STATUS (TABLE) Table III, page 386. C2309 18 15 ENDBIB 13 0 C2309 18 16 NOCOMMON 0 0 C2309 18 17 DATA 8 71 C2309 18 18 EN-MIN EN-MAX ELEMENT MASS ISOMER DATA C2309 18 19 DATA-ERR FLAG C2309 18 20 MEV MEV NO-DIM NO-DIM NO-DIM MB C2309 18 21 MB NO-DIM C2309 18 22 15.6 19.6 38.0 89.0 0.051C2309 18 23 0.01 C2309 18 24 15.6 19.6 38.0 91.0 0.049C2309 18 25 0.01 C2309 18 26 15.6 19.6 40.0 95.0 0.11C2309 18 27 0.04 C2309 18 28 15.6 19.6 40.0 97.0 0.058C2309 18 29 0.02 C2309 18 30 15.6 19.6 48.0 115.0 0.0047C2309 18 31 0.003 C2309 18 32 15.6 19.6 48.0 115.0 0.0052C2309 18 33 0.004 C2309 18 34 15.6 19.6 56.0 140.0 0.037C2309 18 35 0.019 C2309 18 36 25.7 28.9 30.0 72.0 0.036C2309 18 37 0.009 C2309 18 38 25.7 28.9 32.0 77.0 0.083C2309 18 39 0.03 C2309 18 40 25.7 28.9 38.0 89.0 38.0C2309 18 41 19.0 C2309 18 42 25.7 28.9 38.0 91.0 66.0C2309 18 43 33.0 C2309 18 44 25.7 28.9 39.0 93.0 7.4C2309 18 45 3.7 C2309 18 46 25.7 28.9 40.0 95.0 46.0C2309 18 47 9.0 C2309 18 48 25.7 28.9 40.0 97.0 25.0C2309 18 49 5.0 C2309 18 50 25.7 28.9 42.0 99.0 28.0C2309 18 51 6.0 C2309 18 52 25.7 28.9 44.0 103.0 11.0C2309 18 53 2.0 1.0 C2309 18 54 25.7 28.9 44.0 106.0 8.6C2309 18 55 1.7 1.0 C2309 18 56 25.7 28.9 46.0 109.0 8.2C2309 18 57 2.1 C2309 18 58 25.7 28.9 46.0 112.0 8.6C2309 18 59 2.1 C2309 18 60 25.7 28.9 47.0 111.0 11.0C2309 18 61 2.0 C2309 18 62 25.7 28.9 48.0 115.0 0.0 12.0C2309 18 63 4.0 C2309 18 64 25.7 28.9 48.0 115.0 1.0 0.79C2309 18 65 0.2 C2309 18 66 25.7 28.9 48.0 115.0 13.0C2309 18 67 4.0 C2309 18 68 25.7 28.9 53.0 131.0 16.0C2309 18 69 4.0 C2309 18 70 25.7 28.9 53.0 133.0 26.0C2309 18 71 7.0 C2309 18 72 25.7 28.9 56.0 140.0 25.0C2309 18 73 6.0 C2309 18 74 34.9 37.7 30.0 72.0 0.14C2309 18 75 0.03 C2309 18 76 34.9 37.7 32.0 77.0 0.04C2309 18 77 0.02 C2309 18 78 34.9 37.7 35.0 83.0 10.0C2309 18 79 5.0 C2309 18 80 34.9 37.7 38.0 89.0 30.0C2309 18 81 10.0 C2309 18 82 34.9 37.7 38.0 91.0 34.0C2309 18 83 7.0 C2309 18 84 34.9 37.7 40.0 95.0 46.0C2309 18 85 9.0 C2309 18 86 34.9 37.7 40.0 97.0 42.0C2309 18 87 8.0 C2309 18 88 34.9 37.7 42.0 99.0 40.0C2309 18 89 8.0 C2309 18 90 34.9 37.7 44.0 103.0 15.0C2309 18 91 4.0 1.0 C2309 18 92 34.9 37.7 44.0 106.0 16.0C2309 18 93 3.0 1.0 C2309 18 94 34.9 37.7 46.0 109.0 17.0C2309 18 95 3.0 C2309 18 96 34.9 37.7 46.0 112.0 20.0C2309 18 97 4.0 C2309 18 98 34.9 37.7 47.0 111.0 27.0C2309 18 99 5.0 C2309 18 100 34.9 37.7 48.0 115.0 0.0 24.0C2309 18 101 5.0 C2309 18 102 34.9 37.7 48.0 115.0 1.0 1.4C2309 18 103 0.3 C2309 18 104 34.9 37.7 48.0 115.0 25.0C2309 18 105 5.0 C2309 18 106 34.9 37.7 53.0 131.0 22.0C2309 18 107 6.0 C2309 18 108 34.9 37.7 53.0 133.0 34.0C2309 18 109 14.0 C2309 18 110 34.9 37.7 56.0 140.0 30.0C2309 18 111 6.0 C2309 18 112 39.6 42.2 40.0 95.0 8.3C2309 18 113 1.7 C2309 18 114 39.6 42.2 40.0 97.0 7.7C2309 18 115 1.9 C2309 18 116 39.6 42.2 56.0 139.0 42.0C2309 18 117 12.0 C2309 18 118 39.6 42.2 56.0 140.0 37.0C2309 18 119 7.0 C2309 18 120 43.4 45.9 30.0 72.0 0.34C2309 18 121 0.07 C2309 18 122 43.4 45.9 32.0 77.0 0.58C2309 18 123 0.14 C2309 18 124 43.4 45.9 38.0 89.0 27.0C2309 18 125 6.0 C2309 18 126 43.4 45.9 38.0 91.0 30.0C2309 18 127 8.0 C2309 18 128 43.4 45.9 40.0 95.0 91.0C2309 18 129 18.0 C2309 18 130 43.4 45.9 40.0 97.0 73.0C2309 18 131 18.0 C2309 18 132 43.4 45.9 41.0 96.0 0.45C2309 18 133 0.15 C2309 18 134 43.4 45.9 42.0 99.0 56.0C2309 18 135 11.0 C2309 18 136 43.4 45.9 44.0 103.0 24.0C2309 18 137 5.0 1.0 C2309 18 138 43.4 45.9 44.0 105.0 23.0C2309 18 139 8.0 1.0 C2309 18 140 43.4 45.9 44.0 106.0 31.0C2309 18 141 6.0 1.0 C2309 18 142 43.4 45.9 46.0 109.0 38.0C2309 18 143 8.0 C2309 18 144 43.4 45.9 46.0 112.0 33.0C2309 18 145 7.0 C2309 18 146 43.4 45.9 47.0 111.0 63.0C2309 18 147 13.0 C2309 18 148 43.4 45.9 48.0 115.0 0.0 54.0C2309 18 149 27.0 C2309 18 150 43.4 45.9 48.0 115.0 1.0 7.8C2309 18 151 3.9 C2309 18 152 43.4 45.9 48.0 115.0 62.0C2309 18 153 31.0 C2309 18 154 43.4 45.9 56.0 140.0 30.0C2309 18 155 8.0 C2309 18 156 43.4 45.9 58.0 141.0 55.0C2309 18 157 11.0 C2309 18 158 43.4 45.9 58.0 143.0 57.0C2309 18 159 14.0 C2309 18 160 43.4 45.9 58.0 144.0 27.0C2309 18 161 5.0 C2309 18 162 43.4 45.9 60.0 147.0 11.0C2309 18 163 4.0 C2309 18 164 ENDDATA 146 0 C2309 18 165 ENDSUBENT 164 0 C2309 1899999 SUBENT C2309019 20180601 C177C2309 19 1 BIB 5 13 C2309 19 2 REACTION (90-TH-232(A,F)ELEM/MASS,,SIG) Shielded nuclide (one C2309 19 3 whose precursor in the b-decay chain is either stable C2309 19 4 or long-lived). C2309 19 5 SAMPLE A few of the thorium targets were thin uniform depositsC2309 19 6 (~500 microg/cm2) of the hydrated thorium or uranium C2309 19 7 oxide electrodeposited on aluminum. The amount of C2309 19 8 Th232 was determined by alpha counting of the C2309 19 9 resulting thin deposits. C2309 19 10 ERR-ANALYS (DATA-ERR) The limits of fission errors are estimated. C2309 19 11 CORRECTION For thorium, corrections were applied to account for C2309 19 12 the contribution from alpha particle-emitting C2309 19 13 daughters of the Th232. C2309 19 14 STATUS (TABLE) Table III, page 386. C2309 19 15 ENDBIB 13 0 C2309 19 16 NOCOMMON 0 0 C2309 19 17 DATA 6 12 C2309 19 18 EN-MIN EN-MAX ELEMENT MASS DATA DATA-ERR C2309 19 19 MEV MEV NO-DIM NO-DIM MB MB C2309 19 20 25.7 28.9 33.0 77.0 0.12 0.05C2309 19 21 25.7 28.9 35.0 82.0 0.034 0.01C2309 19 22 25.7 28.9 37.0 86.0 1.2 0.5C2309 19 23 25.7 28.9 55.0 136.0 2.8 0.6C2309 19 24 25.7 28.9 57.0 140.0 1.7 0.5C2309 19 25 34.9 37.7 33.0 77.0 0.37 0.11C2309 19 26 34.9 37.7 35.0 82.0 0.3 0.006C2309 19 27 34.9 37.7 37.0 86.0 0.034 0.009C2309 19 28 34.9 37.7 55.0 136.0 7.1 1.4C2309 19 29 43.4 45.9 37.0 86.0 0.099 0.025C2309 19 30 43.4 45.9 55.0 136.0 17.0 4.0C2309 19 31 43.4 45.9 57.0 140.0 3.7 1.C2309 19 32 ENDDATA 14 0 C2309 19 33 ENDSUBENT 32 0 C2309 1999999 SUBENT C2309020 20180606 C177C2309 20 1 BIB 6 12 C2309 20 2 REACTION (90-TH-232(A,F)ELEM/MASS,CUM,SIG) C2309 20 3 SAMPLE A few of the thorium targets were thin uniform depositsC2309 20 4 (~500 microg/cm2) of the hydrated thorium or uranium C2309 20 5 oxide electrodeposited on aluminum. The amount of C2309 20 6 Th232 was determined by alpha counting of the C2309 20 7 resulting thin deposits. C2309 20 8 ERR-ANALYS (DATA-ERR) The limits of fission errors are estimated. C2309 20 9 FLAG (1.) Contribution from Cd115m estimated. C2309 20 10 CORRECTION For thorium, corrections were applied to account for C2309 20 11 the contribution from alpha particle-emitting C2309 20 12 daughters of the Th232. C2309 20 13 STATUS (TABLE) Table III, page 386. C2309 20 14 ENDBIB 12 0 C2309 20 15 COMMON 1 3 C2309 20 16 EN-ERR C2309 20 17 MEV C2309 20 18 0.5 C2309 20 19 ENDCOMMON 3 0 C2309 20 20 DATA 7 8 C2309 20 21 EN ELEMENT MASS ISOMER DATA DATA-ERR C2309 20 22 FLAG C2309 20 23 MEV NO-DIM NO-DIM NO-DIM MB MB C2309 20 24 NO-DIM C2309 20 25 19.8 38.0 89.0 0.84 0.2C2309 20 26 C2309 20 27 19.8 38.0 91.0 0.96 0.32C2309 20 28 C2309 20 29 19.8 40.0 95.0 1.1 0.2C2309 20 30 C2309 20 31 19.8 40.0 97.0 1.1 0.2C2309 20 32 C2309 20 33 19.8 48.0 115.0 0.0 0.3 0.2C2309 20 34 C2309 20 35 19.8 48.0 115.0 0.32 0.31C2309 20 36 1.0 C2309 20 37 19.8 56.0 139.0 0.77 0.3C2309 20 38 C2309 20 39 19.8 56.0 140.0 0.82 0.2C2309 20 40 C2309 20 41 ENDDATA 20 0 C2309 20 42 ENDSUBENT 41 0 C2309 2099999 SUBENT C2309021 20180606 C177C2309 21 1 BIB 7 22 C2309 21 2 REACTION (90-TH-232(A,F)MASS,CHN,SIG) C2309 21 3 SAMPLE A few of the thorium targets were thin uniform depositsC2309 21 4 (~500 microg/cm2) of the hydrated thorium or uranium C2309 21 5 oxide electrodeposited on aluminum. The amount of C2309 21 6 Th232 was determined by alpha counting of the C2309 21 7 resulting thin deposits. C2309 21 8 ANALYSIS Most of the values for the chain yields are identical C2309 21 9 to those for the cumulative yields of the nuclide C2309 21 10 given in the other subentry, except that (some) cross C2309 21 11 sections were increased by "a small amount" to account C2309 21 12 for fission products of the same mass chain not C2309 21 13 included experimentally. C2309 21 14 ERR-ANALYS (DATA-ERR) The limits fission errors are estimated. C2309 21 15 FLAG (1.) Contribution from Cd115m estimated. C2309 21 16 (3.) The cross section for formation of the daughter C2309 21 17 was measured and found negligible. C2309 21 18 (4.) Isotopic-exchange difficulties which make C2309 21 19 ruthenium cross sections unreliable. C2309 21 20 CORRECTION For thorium, corrections were applied to account for C2309 21 21 the contribution from alpha particle-emitting C2309 21 22 daughters of the Th232. C2309 21 23 STATUS (TABLE) Table III, page 386. C2309 21 24 ENDBIB 22 0 C2309 21 25 NOCOMMON 0 0 C2309 21 26 DATA 6 63 C2309 21 27 EN-MIN EN-MAX MASS DATA DATA-ERR FLAG C2309 21 28 MEV MEV NO-DIM MB MB NO-DIM C2309 21 29 15.6 19.6 89.0 0.051 0.01 C2309 21 30 15.6 19.6 91.0 0.049 0.01 C2309 21 31 15.6 19.6 95.0 0.11 0.04 C2309 21 32 15.6 19.6 97.0 0.059 0.02 C2309 21 33 15.6 19.6 115.0 0.0052 0.004 C2309 21 34 15.6 19.6 140.0 0.042 0.021 C2309 21 35 25.7 28.9 72.0 0.038 0.01 C2309 21 36 25.7 28.9 77.0 0.2 0.1 C2309 21 37 25.7 28.9 89.0 38.0 19.0 C2309 21 38 25.7 28.9 91.0 66.0 33.0 3.0C2309 21 39 25.7 28.9 93.0 7.4 3.7 C2309 21 40 25.7 28.9 95.0 46.0 9.0 3.0C2309 21 41 25.7 28.9 97.0 25.0 5.0 C2309 21 42 25.7 28.9 99.0 28.0 6.0 C2309 21 43 25.7 28.9 103.0 11.0 0.2 4.0C2309 21 44 25.7 28.9 106.0 8.7 1.8 4.0C2309 21 45 25.7 28.9 109.0 8.2 2.1 C2309 21 46 25.7 28.9 111.0 11.0 2.0 C2309 21 47 25.7 28.9 112.0 8.8 2.2 C2309 21 48 25.7 28.9 115.0 13.0 4.0 C2309 21 49 25.7 28.9 131.0 17.0 5.0 C2309 21 50 25.7 28.9 133.0 32.0 9.0 C2309 21 51 25.7 28.9 140.0 27.0 7.0 C2309 21 52 34.9 37.7 72.0 0.15 0.04 C2309 21 53 34.9 37.7 77.0 0.41 0.13 C2309 21 54 34.9 37.7 83.0 10.0 5.0 C2309 21 55 34.9 37.7 89.0 30.0 10.0 C2309 21 56 34.9 37.7 91.0 35.0 8.0 C2309 21 57 34.9 37.7 95.0 46.0 9.0 3.0C2309 21 58 34.9 37.7 97.0 45.0 9.0 C2309 21 59 34.9 37.7 99.0 41.0 9.0 C2309 21 60 34.9 37.7 103.0 15.0 4.0 4.0C2309 21 61 34.9 37.7 106.0 17.0 4.0 4.0C2309 21 62 34.9 37.7 109.0 17.0 3.0 C2309 21 63 34.9 37.7 111.0 27.0 5.0 C2309 21 64 34.9 37.7 112.0 21.0 4.0 C2309 21 65 34.9 37.7 115.0 25.0 5.0 C2309 21 66 34.9 37.7 131.0 26.0 6.0 C2309 21 67 34.9 37.7 133.0 52.0 25.0 C2309 21 68 34.9 37.7 140.0 42.0 8.0 C2309 21 69 39.6 42.2 95.0 8.4 1.7 C2309 21 70 39.6 42.2 97.0 8.2 2.1 C2309 21 71 39.6 42.2 139.0 50.0 16.0 C2309 21 72 39.6 42.2 140.0 52.0 11.0 C2309 21 73 43.4 45.9 72.0 0.37 0.09 C2309 21 74 43.4 45.9 77.0 0.58 0.14 3.0C2309 21 75 43.4 45.9 89.0 27.0 6.0 C2309 21 76 43.4 45.9 91.0 30.0 8.0 3.0C2309 21 77 43.4 45.9 95.0 91.0 18.0 3.0C2309 21 78 43.4 45.9 97.0 76.0 20.0 C2309 21 79 43.4 45.9 99.0 56.0 11.0 C2309 21 80 43.4 45.9 103.0 24.0 5.0 4.0C2309 21 81 43.4 45.9 105.0 23.0 8.0 4.0C2309 21 82 43.4 45.9 106.0 32.0 6.0 4.0C2309 21 83 43.4 45.9 109.0 38.0 8.0 C2309 21 84 43.4 45.9 111.0 63.0 13.0 C2309 21 85 43.4 45.9 112.0 36.0 7.0 C2309 21 86 43.4 45.9 115.0 63.0 33.0 C2309 21 87 43.4 45.9 140.0 34.0 9.0 C2309 21 88 43.4 45.9 141.0 58.0 13.0 C2309 21 89 43.4 45.9 143.0 57.0 14.0 3.0C2309 21 90 43.4 45.9 144.0 35.0 8.0 C2309 21 91 43.4 45.9 147.0 12.0 5.0 C2309 21 92 ENDDATA 65 0 C2309 21 93 ENDSUBENT 92 0 C2309 2199999 SUBENT C2309022 20180606 C177C2309 22 1 BIB 7 16 C2309 22 2 REACTION (90-TH-232(A,F)MASS,CHN,SIG) C2309 22 3 SAMPLE An electroplated target. The amount of Th232 was C2309 22 4 determined by alpha counting of the resulting thin C2309 22 5 deposits. C2309 22 6 ANALYSIS Most of the values for the chain yields are identical C2309 22 7 to those for the cumulative yields of the nuclide C2309 22 8 given in the other subentry, except that (some) cross C2309 22 9 sections were increased by "a small amount" to account C2309 22 10 for fission products of the same mass chain not C2309 22 11 included experimentally. C2309 22 12 ERR-ANALYS (DATA-ERR) The limits of fission errors are estimated. C2309 22 13 FLAG (1.) Contribution from Cd115m estimated. C2309 22 14 CORRECTION For thorium, corrections were applied to account for C2309 22 15 the contribution from alpha particle-emitting C2309 22 16 daughters of the Th232. C2309 22 17 STATUS (TABLE) Table III, page 386. C2309 22 18 ENDBIB 16 0 C2309 22 19 COMMON 1 3 C2309 22 20 EN-ERR C2309 22 21 MEV C2309 22 22 0.5 C2309 22 23 ENDCOMMON 3 0 C2309 22 24 DATA 5 7 C2309 22 25 EN MASS DATA DATA-ERR FLAG C2309 22 26 MEV NO-DIM MB MB NO-DIM C2309 22 27 19.8 89.0 0.84 0.2 C2309 22 28 19.8 91.0 0.96 0.32 C2309 22 29 19.8 95.0 1.1 0.2 C2309 22 30 19.8 97.0 1.1 0.2 C2309 22 31 19.8 115.0 0.32 0.31 1.0 C2309 22 32 19.8 139.0 0.85 0.3 C2309 22 33 19.8 140.0 0.96 0.2 C2309 22 34 ENDDATA 9 0 C2309 22 35 ENDSUBENT 34 0 C2309 2299999 SUBENT C2309023 20180606 C177C2309 23 1 BIB 5 11 C2309 23 2 REACTION (90-TH-232(A,F)MASS,CHN,SIG) C2309 23 3 SAMPLE A few of the thorium targets were thin uniform depositsC2309 23 4 (~500 microg/cm2) of the hydrated thorium or uranium C2309 23 5 oxide electrodeposited on aluminum. The amount of C2309 23 6 Th232 was determined by alpha counting of the C2309 23 7 resulting thin deposits. C2309 23 8 ERR-ANALYS (DATA-ERR) The limits of fission errors are estimated. C2309 23 9 CORRECTION For thorium, corrections were applied to account for C2309 23 10 the contribution from alpha particle-emitting C2309 23 11 daughters of the Th232. C2309 23 12 STATUS (TABLE) Table III, page 386. C2309 23 13 ENDBIB 11 0 C2309 23 14 NOCOMMON 0 0 C2309 23 15 DATA 5 4 C2309 23 16 EN-MIN EN-MAX MASS DATA DATA-ERR C2309 23 17 MEV MEV NO-DIM MB MB C2309 23 18 25.7 28.9 77.0 0.2 0.1 C2309 23 19 25.7 28.9 140.0 28.0 7.0 C2309 23 20 34.9 37.7 77.0 0.41 0.13 C2309 23 21 43.4 45.9 140.0 38.0 10.0 C2309 23 22 ENDDATA 6 0 C2309 23 23 ENDSUBENT 22 0 C2309 2399999 SUBENT C2309024 20180606 C177C2309 24 1 BIB 3 9 C2309 24 2 REACTION (90-TH-232(A,F),,SIG) C2309 24 3 ERR-ANALYS (DATA-ERR) The limits of fission errors are estimated. C2309 24 4 STATUS (DEP,C2309004) C2309 24 5 (DEP,C2309005) C2309 24 6 (DEP,C2309006) C2309 24 7 (DEP,C2309007) C2309 24 8 (DEP,C2309008) C2309 24 9 (DEP,C2309009) C2309 24 10 (TABLE) Table III, page 386. C2309 24 11 ENDBIB 9 0 C2309 24 12 NOCOMMON 0 0 C2309 24 13 DATA 4 4 C2309 24 14 EN-MIN EN-MAX DATA DATA-ERR C2309 24 15 MEV MEV MB MB C2309 24 16 15.6 19.6 0.93 0.24 C2309 24 17 25.7 28.9 590.0 150.0 C2309 24 18 34.9 37.7 930.0 240.0 C2309 24 19 43.4 45.9 1660.0 410.0 C2309 24 20 ENDDATA 6 0 C2309 24 21 ENDSUBENT 20 0 C2309 2499999 SUBENT C2309025 20180607 C177C2309 25 1 BIB 4 8 C2309 25 2 REACTION (92-U-233(D,F)ELEM/MASS,CUM,SIG) C2309 25 3 SAMPLE (92-U-233,ENR=0.96) C2309 25 4 (92-U-238,ENR=0.03) and U-234 < 1%. An electroplated C2309 25 5 target. The amount of U233 was determined by alpha C2309 25 6 counting of the resulting thin deposits. C2309 25 7 ERR-ANALYS (DATA-ERR,20.,30.) The limits of erors are estimated C2309 25 8 to be about 20 to 30%. C2309 25 9 STATUS (TABLE) Table IV, page 388. C2309 25 10 ENDBIB 8 0 C2309 25 11 COMMON 1 3 C2309 25 12 EN-ERR C2309 25 13 MEV C2309 25 14 0.5 C2309 25 15 ENDCOMMON 3 0 C2309 25 16 DATA 6 71 C2309 25 17 EN ELEMENT MASS ISOMER DATA DATA-MAX C2309 25 18 MEV NO-DIM NO-DIM NO-DIM MB MB C2309 25 19 9.0 38.0 89.0 4.59 C2309 25 20 9.0 38.0 91.0 3.90 C2309 25 21 9.0 40.0 95.0 6.45 C2309 25 22 9.0 40.0 97.0 4.59 C2309 25 23 9.0 44.0 105.0 5.03 C2309 25 24 9.0 48.0 115.0 0.0 1.22 C2309 25 25 9.0 48.0 115.0 1.34 C2309 25 26 9.0 48.0 117.0 1.70 C2309 25 27 9.0 56.0 139.0 4.26 C2309 25 28 9.0 56.0 140.0 3.50 C2309 25 29 12.1 38.0 89.0 14.4 C2309 25 30 12.1 38.0 91.0 23.1 C2309 25 31 12.1 40.0 97.0 25.6 C2309 25 32 12.1 48.0 115.0 0.0 8.43 C2309 25 33 12.1 48.0 115.0 1.0 1.55C2309 25 34 12.1 48.0 115.0 9.98 C2309 25 35 12.1 48.0 117.0 12.1 C2309 25 36 12.1 56.0 139.0 20.4 C2309 25 37 12.1 56.0 140.0 17.1 C2309 25 38 14.0 38.0 89.0 18.9 C2309 25 39 14.0 38.0 91.0 18.7 C2309 25 40 14.0 40.0 95.0 44.8 C2309 25 41 14.0 40.0 97.0 39.3 C2309 25 42 14.0 48.0 115.0 0.0 14.7 C2309 25 43 14.0 48.0 115.0 1.0 1.97C2309 25 44 14.0 48.0 115.0 16.1 C2309 25 45 14.0 48.0 117.0 19.5 C2309 25 46 14.0 56.0 140.0 21.8 C2309 25 47 15.4 38.0 89.0 26.4 C2309 25 48 15.4 38.0 91.0 31.0 C2309 25 49 15.4 48.0 115.0 0.0 22.9 C2309 25 50 15.4 48.0 115.0 1.0 3.92C2309 25 51 15.4 48.0 115.0 26.8 C2309 25 52 15.4 48.0 117.0 21.9 C2309 25 53 15.4 56.0 139.0 39.3 C2309 25 54 15.4 56.0 140.0 29.2 C2309 25 55 19.6 38.0 89.0 46.5 C2309 25 56 19.6 38.0 91.0 36.9 C2309 25 57 19.6 40.0 95.0 58.5 C2309 25 58 19.6 40.0 97.0 49.8 C2309 25 59 19.6 48.0 115.0 0.0 44.0 C2309 25 60 19.6 48.0 115.0 1.0 5.58C2309 25 61 19.6 48.0 115.0 49.6 C2309 25 62 19.6 48.0 117.0 41.8 C2309 25 63 19.6 56.0 139.0 49.2 C2309 25 64 19.6 56.0 140.0 37.5 C2309 25 65 21.5 38.0 89.0 34.6 C2309 25 66 21.5 38.0 91.0 52.5 C2309 25 67 21.5 40.0 95.0 61.6 C2309 25 68 21.5 40.0 97.0 61.8 C2309 25 69 21.5 46.0 109.0 46.7 C2309 25 70 21.5 46.0 112.0 52.9 C2309 25 71 21.5 48.0 115.0 0.0 47.3 C2309 25 72 21.5 48.0 115.0 1.0 8.5C2309 25 73 21.5 48.0 115.0 55.8 C2309 25 74 21.5 48.0 117.0 50.0 C2309 25 75 21.5 56.0 139.0 46.5 C2309 25 76 21.5 56.0 140.0 35.5 C2309 25 77 23.4 38.0 89.0 42.7 C2309 25 78 23.4 38.0 91.0 44.3 C2309 25 79 23.4 40.0 95.0 54.2 C2309 25 80 23.4 40.0 97.0 53.5 C2309 25 81 23.4 48.0 115.0 0.0 63.9 C2309 25 82 23.4 48.0 115.0 1.0 4.8C2309 25 83 23.4 48.0 115.0 68.7 C2309 25 84 23.4 48.0 117.0 59.0 C2309 25 85 23.4 56.0 139.0 34.0 C2309 25 86 23.4 56.0 140.0 31.5 C2309 25 87 23.4 60.0 147.0 12.2 C2309 25 88 23.4 63.0 157.0 0.76 C2309 25 89 23.4 64.0 159.0 0.54 C2309 25 90 ENDDATA 73 0 C2309 25 91 ENDSUBENT 90 0 C2309 2599999 SUBENT C2309026 20180607 C177C2309 26 1 BIB 4 8 C2309 26 2 REACTION (92-U-233(D,F)MASS,CHN,SIG) C2309 26 3 SAMPLE (92-U-233,ENR=0.96) C2309 26 4 (92-U-238,ENR=0.03) and U-234 < 1%. An electroplated C2309 26 5 target. The amount of U233 was determined by alpha C2309 26 6 counting of the resulting thin deposits. C2309 26 7 ERR-ANALYS (DATA-ERR,20.,30.) The limits of erors are estimated C2309 26 8 to be about 20 to 30%. C2309 26 9 STATUS (TABLE) Table IV, page 388. C2309 26 10 ENDBIB 8 0 C2309 26 11 COMMON 1 3 C2309 26 12 EN-ERR C2309 26 13 MEV C2309 26 14 0.5 C2309 26 15 ENDCOMMON 3 0 C2309 26 16 DATA 5 71 C2309 26 17 EN MASS ISOMER DATA DATA-MAX C2309 26 18 MEV NO-DIM NO-DIM MB MB C2309 26 19 9.0 89.0 4.64 C2309 26 20 9.0 91.0 4.01 C2309 26 21 9.0 95.0 6.55 C2309 26 22 9.0 97.0 4.80 C2309 26 23 9.0 105.0 5.11 C2309 26 24 9.0 115.0 0.0 1.24 C2309 26 25 9.0 115.0 1.36 C2309 26 26 9.0 117.0 1.78 C2309 26 27 9.0 139.0 4.82 C2309 26 28 9.0 140.0 4.27 C2309 26 29 12.1 89.0 14.6 C2309 26 30 12.1 91.0 23.8 C2309 26 31 12.1 97.0 26.8 C2309 26 32 12.1 115.0 0.0 8.57 C2309 26 33 12.1 115.0 1.0 1.58 C2309 26 34 12.1 115.0 10.2 C2309 26 35 12.1 117.0 12.5 C2309 26 36 12.1 139.0 23.1 C2309 26 37 12.1 140.0 20.9 C2309 26 38 14.0 89.0 19.1 C2309 26 39 14.0 91.0 19.2 C2309 26 40 14.0 95.0 45.6 C2309 26 41 14.0 97.0 41.1 C2309 26 42 14.0 115.0 0.0 15.0 C2309 26 43 14.0 115.0 1.0 2.0 C2309 26 44 14.0 115.0 17.0 C2309 26 45 14.0 117.0 20.4 C2309 26 46 14.0 140.0 26.6 C2309 26 47 15.4 89.0 26.7 C2309 26 48 15.4 91.0 32.0 C2309 26 49 15.4 115.0 0.0 23.4 C2309 26 50 15.4 115.0 1.0 4.0 C2309 26 51 15.4 115.0 27.4 C2309 26 52 15.4 117.0 23.2 C2309 26 53 15.4 139.0 46.2 C2309 26 54 15.4 140.0 41.7 C2309 26 55 19.6 89.0 48.2 C2309 26 56 19.6 91.0 38.0 C2309 26 57 19.6 95.0 59.7 C2309 26 58 19.6 97.0 52.4 C2309 26 59 19.6 115.0 0.0 45.0 C2309 26 60 19.6 115.0 1.0 5.70 C2309 26 61 19.6 115.0 50.7 C2309 26 62 19.6 117.0 44.2 C2309 26 63 19.6 139.0 57.9 C2309 26 64 19.6 140.0 53.6 C2309 26 65 21.5 89.0 35.1 C2309 26 66 21.5 91.0 54.6 C2309 26 67 21.5 95.0 63.0 C2309 26 68 21.5 97.0 66.0 C2309 26 69 21.5 109.0 47.5 C2309 26 70 21.5 112.0 56.9 C2309 26 71 21.5 115.0 0.0 48.6 C2309 26 72 21.5 115.0 1.0 8.7 C2309 26 73 21.5 115.0 57.3 C2309 26 74 21.5 117.0 53.8 C2309 26 75 21.5 139.0 58.1 C2309 26 76 21.5 140.0 53.0 C2309 26 77 23.4 89.0 43.3 C2309 26 78 23.4 91.0 46.2 C2309 26 79 23.4 95.0 55.5 C2309 26 80 23.4 97.0 57.2 C2309 26 81 23.4 115.0 0.0 65.7 C2309 26 82 23.4 115.0 1.0 4.9 C2309 26 83 23.4 115.0 70.6 C2309 26 84 23.4 117.0 63.5 C2309 26 85 23.4 139.0 45.3 C2309 26 86 23.4 140.0 47.0 C2309 26 87 23.4 147.0 13.3 C2309 26 88 23.4 157.0 1.03 C2309 26 89 23.4 159.0 0.70 C2309 26 90 ENDDATA 73 0 C2309 26 91 ENDSUBENT 90 0 C2309 2699999 SUBENT C2309027 20180607 C177C2309 27 1 BIB 4 9 C2309 27 2 REACTION (92-U-233(D,F),,SIG) C2309 27 3 SAMPLE (92-U-233,ENR=0.96) C2309 27 4 (92-U-238,ENR=0.03) and U-234 < 1%. An electroplated C2309 27 5 target. The amount of U233 was determined by alpha C2309 27 6 counting of the resulting thin deposits. C2309 27 7 ERR-ANALYS (DATA-ERR) The limits of fission errors are estimated. C2309 27 8 STATUS (DEP,C2309012) C2309 27 9 (DEP,C2309013) C2309 27 10 (TABLE) Table IV, page 388. C2309 27 11 ENDBIB 9 0 C2309 27 12 NOCOMMON 0 0 C2309 27 13 DATA 3 7 C2309 27 14 EN DATA DATA-ERR C2309 27 15 MEV MB MB C2309 27 16 9.0 125.0 34.0 C2309 27 17 12.1 605.0 163.0 C2309 27 18 14.0 857.0 231.0 C2309 27 19 15.4 1093.0 295.0 C2309 27 20 19.6 1502.0 406.0 C2309 27 21 21.5 1687.0 456.0 C2309 27 22 23.4 1861.0 503.0 C2309 27 23 ENDDATA 9 0 C2309 27 24 ENDSUBENT 23 0 C2309 2799999 ENDENTRY 27 0 C230999999999