ENTRY C2296 20241031 C243C229600000001 SUBENT C2296001 20241031 C243C229600100001 BIB 7 17 C229600100002 TITLE Spallation-Fission Competition in Heaviest Elements; C229600100003 Helium-Ion-Induced Reactions in Plutonium Isotopes C229600100004 AUTHOR (R.A.Glass,R.J.Carr,J.W.Cobble,G.T.Seaborg) C229600100005 REFERENCE (J,PR,104,434,1956) C229600100006 #doi:10.1103/PhysRev.104.434 C229600100007 INSTITUTE (1USABRK,1USAUCX) C229600100008 FACILITY (LINAC,1USABRK) C229600100009 (CYCLO,1USABRK) Bombardments with helium ions of C229600100010 energy up to about 50 MeV and deuterons up to about C229600100011 25-MeV energy are performed on the 60-inch cyclotron C229600100012 of the Crocker Laboratory. C229600100013 METHOD (CHSEP,ACTIV) The method employed consists of C229600100014 cyclotron bombardments of plutonium oxide followed by C229600100015 the chemical isolation and alpha or beta counting of C229600100016 radioactive reaction products. C229600100017 HISTORY (20180511C) BP C229600100018 (20241028A) OS. DECAY-DATA in subs.4,18 corrected C229600100019 ENDBIB 17 0 C229600100020 NOCOMMON 0 0 C229600100021 ENDSUBENT 20 0 C229600199999 SUBENT C2296002 20180511 C175C2296 2 1 BIB 5 13 C2296 2 2 REACTION (94-PU-238(A,N)96-CM-241,,SIG) C2296 2 3 SAMPLE (94-PU-238,ENR=0.938) C2296 2 4 (94-PU-239,ENR=0.058) and small amounts of C2296 2 5 Pu-240,Pu-241 and Pu-242. C2296 2 6 ERR-ANALYS (ERR-T) These errors can be combined to give the C2296 2 7 following average total errors. C2296 2 8 (ERR-1,1.,5.) integrated beam intensity. C2296 2 9 (ERR-2) electroplated target density. C2296 2 10 (ERR-3,20.,25.) disintegration rates for electron- C2296 2 11 capture-unstable products, due mainly to counting C2296 2 12 efficiency uncertainties. C2296 2 13 DECAY-DATA (96-CM-241,35.0D,EC) C2296 2 14 STATUS (TABLE) Table I, page 438. C2296 2 15 ENDBIB 13 0 C2296 2 16 COMMON 2 3 C2296 2 17 ERR-T ERR-2 C2296 2 18 PER-CENT PER-CENT C2296 2 19 25.0 10.0 C2296 2 20 ENDCOMMON 3 0 C2296 2 21 DATA 2 6 C2296 2 22 EN DATA C2296 2 23 MEV MB C2296 2 24 25.2 4.6 C2296 2 25 28.7 7.1 C2296 2 26 33.0 6.0 C2296 2 27 36.6 3.1 C2296 2 28 42.2 2.5 C2296 2 29 47.4 2.8 C2296 2 30 ENDDATA 8 0 C2296 2 31 ENDSUBENT 30 0 C2296 299999 SUBENT C2296003 20180511 C175C2296 3 1 BIB 5 12 C2296 3 2 REACTION (94-PU-238(A,2N)96-CM-240,,SIG) C2296 3 3 SAMPLE (94-PU-238,ENR=0.938) C2296 3 4 (94-PU-239,ENR=0.058) and small amounts of C2296 3 5 Pu-240,Pu-241 and Pu-242. C2296 3 6 ERR-ANALYS (ERR-T) These errors can be combined to give the C2296 3 7 following average total errors. C2296 3 8 (ERR-1,1.,5.) integrated beam intensity. C2296 3 9 (ERR-2) electroplated target density. C2296 3 10 (ERR-3) disintegration rates for alpha particle- C2296 3 11 emitting spallation products. C2296 3 12 DECAY-DATA (96-CM-240,27.0D,A) C2296 3 13 STATUS (TABLE) Table I, page 438. C2296 3 14 ENDBIB 12 0 C2296 3 15 COMMON 3 3 C2296 3 16 ERR-T ERR-2 ERR-3 C2296 3 17 PER-CENT PER-CENT PER-CENT C2296 3 18 15.0 10.0 10.0 C2296 3 19 ENDCOMMON 3 0 C2296 3 20 DATA 2 7 C2296 3 21 EN DATA C2296 3 22 MEV MB C2296 3 23 25.2 15.0 C2296 3 24 28.7 14.0 C2296 3 25 30.2 9.9 C2296 3 26 33.0 8.9 C2296 3 27 36.6 4.7 C2296 3 28 42.2 4.3 C2296 3 29 47.4 3.5 C2296 3 30 ENDDATA 9 0 C2296 3 31 ENDSUBENT 30 0 C2296 399999 SUBENT C2296004 20241031 C243C229600400001 BIB 6 14 C229600400002 REACTION (94-PU-238(A,4N)96-CM-238,,SIG) C229600400003 SAMPLE (94-PU-238,ENR=0.938) C229600400004 (94-PU-239,ENR=0.058) and small amounts of C229600400005 Pu-240,Pu-241 and Pu-242. C229600400006 ERR-ANALYS (ERR-T) These errors can be combined to give the C229600400007 following average total errors. C229600400008 (ERR-1,1.,5.) integrated beam intensity. C229600400009 (ERR-2) electroplated target density. C229600400010 (ERR-3,20.,25.) disintegration rates for electron- C229600400011 capture-unstable products, due mainly to counting C229600400012 efficiency uncertainties. C229600400013 DECAY-DATA (96-CM-238,2.5HR,A,,0.018) C229600400014 STATUS (TABLE,,R.A.Glass+,J,PR,104,434,1956) Tab.I, p.438. C229600400015 HISTORY (20241028A) DECAY-DATA: Radiation field replaced C229600400016 ENDBIB 14 0 C229600400017 COMMON 2 3 C229600400018 ERR-T ERR-2 C229600400019 PER-CENT PER-CENT C229600400020 25.0 10.0 C229600400021 ENDCOMMON 3 0 C229600400022 DATA 2 3 C229600400023 EN DATA C229600400024 MEV MB C229600400025 36.6 0.002 C229600400026 42.2 0.19 C229600400027 47.4 0.26 C229600400028 ENDDATA 5 0 C229600400029 ENDSUBENT 28 0 C229600499999 SUBENT C2296005 20180511 C175C2296 5 1 BIB 5 13 C2296 5 2 REACTION (94-PU-238(A,X)95-AM-240,,SIG) C2296 5 3 SAMPLE (94-PU-238,ENR=0.938) C2296 5 4 (94-PU-239,ENR=0.058) and small amounts of C2296 5 5 Pu-240,Pu-241 and Pu-242. C2296 5 6 ERR-ANALYS (ERR-T) These errors can be combined to give the C2296 5 7 following average total errors. C2296 5 8 (ERR-1,1.,5.) integrated beam intensity. C2296 5 9 (ERR-2) electroplated target density. C2296 5 10 (ERR-3,20.,25.) disintegration rates for electron- C2296 5 11 capture-unstable products, due mainly to counting C2296 5 12 efficiency uncertainties. C2296 5 13 DECAY-DATA (95-AM-240,51.0HR,EC) C2296 5 14 STATUS (TABLE) Table I, page 438. C2296 5 15 ENDBIB 13 0 C2296 5 16 COMMON 2 3 C2296 5 17 ERR-T ERR-2 C2296 5 18 PER-CENT PER-CENT C2296 5 19 25.0 10.0 C2296 5 20 ENDCOMMON 3 0 C2296 5 21 DATA 2 6 C2296 5 22 EN DATA C2296 5 23 MEV MB C2296 5 24 28.7 2.6 C2296 5 25 30.2 1.9 C2296 5 26 33.0 3.3 C2296 5 27 36.6 15.0 C2296 5 28 42.2 13.0 C2296 5 29 47.4 8.0 C2296 5 30 ENDDATA 8 0 C2296 5 31 ENDSUBENT 30 0 C2296 599999 SUBENT C2296006 20180511 C175C2296 6 1 BIB 5 13 C2296 6 2 REACTION (94-PU-238(A,X)95-AM-239,CUM,SIG) C2296 6 3 SAMPLE (94-PU-238,ENR=0.938) C2296 6 4 (94-PU-239,ENR=0.058) and small amounts of C2296 6 5 Pu-240,Pu-241 and Pu-242. C2296 6 6 ERR-ANALYS (ERR-T) These errors can be combined to give the C2296 6 7 following average total errors. C2296 6 8 (ERR-1,1.,5.) integrated beam intensity. C2296 6 9 (ERR-2) electroplated target density. C2296 6 10 (ERR-3,20.,25.) disintegration rates for electron- C2296 6 11 capture-unstable products, due mainly to counting C2296 6 12 efficiency uncertainties. C2296 6 13 DECAY-DATA (95-AM-239,12.0HR,EC) C2296 6 14 STATUS (TABLE) Table I, page 438. C2296 6 15 ENDBIB 13 0 C2296 6 16 COMMON 2 3 C2296 6 17 ERR-T ERR-2 C2296 6 18 PER-CENT PER-CENT C2296 6 19 25.0 10.0 C2296 6 20 ENDCOMMON 3 0 C2296 6 21 DATA 2 6 C2296 6 22 EN DATA C2296 6 23 MEV MB C2296 6 24 28.7 3.0 C2296 6 25 30.2 5.2 C2296 6 26 33.0 6.9 C2296 6 27 36.6 27.0 C2296 6 28 42.2 22.0 C2296 6 29 47.4 18.0 C2296 6 30 ENDDATA 8 0 C2296 6 31 ENDSUBENT 30 0 C2296 699999 SUBENT C2296007 20180511 C175C2296 7 1 BIB 4 12 C2296 7 2 REACTION (94-PU-238(A,F)38-SR-91,(CUM),SIG) C2296 7 3 SAMPLE (94-PU-238,ENR=0.938) C2296 7 4 (94-PU-239,ENR=0.058) and small amounts of C2296 7 5 Pu-240,Pu-241 and Pu-242. C2296 7 6 ERR-ANALYS (ERR-T) These errors can be combined to give the C2296 7 7 following average total errors. C2296 7 8 (ERR-1,1.,5.) integrated beam intensity. C2296 7 9 (ERR-2) electroplated target density. C2296 7 10 (ERR-3,20.,25.) disintegration rates for negatron- C2296 7 11 emitting fission products, due mainly to counting C2296 7 12 correction uncertainties. C2296 7 13 STATUS (TABLE) Table I, page 438. C2296 7 14 ENDBIB 12 0 C2296 7 15 COMMON 2 3 C2296 7 16 ERR-T ERR-2 C2296 7 17 PER-CENT PER-CENT C2296 7 18 25.0 10.0 C2296 7 19 ENDCOMMON 3 0 C2296 7 20 DATA 2 5 C2296 7 21 EN DATA C2296 7 22 MEV MB C2296 7 23 28.7 14.0 C2296 7 24 33.0 17.0 C2296 7 25 36.6 12.0 C2296 7 26 42.2 11.0 C2296 7 27 47.4 29.0 C2296 7 28 ENDDATA 7 0 C2296 7 29 ENDSUBENT 28 0 C2296 799999 SUBENT C2296008 20180511 C175C2296 8 1 BIB 4 12 C2296 8 2 REACTION (94-PU-238(A,F)48-CD-115,(CUM),SIG) M+G C2296 8 3 SAMPLE (94-PU-238,ENR=0.938) C2296 8 4 (94-PU-239,ENR=0.058) and small amounts of C2296 8 5 Pu-240,Pu-241 and Pu-242. C2296 8 6 ERR-ANALYS (ERR-T) These errors can be combined to give the C2296 8 7 following average total errors. C2296 8 8 (ERR-1,1.,5.) integrated beam intensity. C2296 8 9 (ERR-2) electroplated target density. C2296 8 10 (ERR-3,20.,25.) disintegration rates for negatron- C2296 8 11 emitting fission products, due mainly to counting C2296 8 12 correction uncertainties. C2296 8 13 STATUS (TABLE) Table I, page 438. C2296 8 14 ENDBIB 12 0 C2296 8 15 COMMON 2 3 C2296 8 16 ERR-T ERR-2 C2296 8 17 PER-CENT PER-CENT C2296 8 18 25.0 10.0 C2296 8 19 ENDCOMMON 3 0 C2296 8 20 DATA 2 7 C2296 8 21 EN DATA C2296 8 22 MEV MB C2296 8 23 25.2 10.0 C2296 8 24 28.7 23.0 C2296 8 25 30.2 28.0 C2296 8 26 33.0 43.0 C2296 8 27 36.6 38.0 C2296 8 28 42.2 43.0 C2296 8 29 47.4 57.0 C2296 8 30 ENDDATA 9 0 C2296 8 31 ENDSUBENT 30 0 C2296 899999 SUBENT C2296009 20180511 C175C2296 9 1 BIB 4 12 C2296 9 2 REACTION (94-PU-238(A,F)56-BA-140,(CUM),SIG) C2296 9 3 SAMPLE (94-PU-238,ENR=0.938) C2296 9 4 (94-PU-239,ENR=0.058) and small amounts of C2296 9 5 Pu-240,Pu-241 and Pu-242. C2296 9 6 ERR-ANALYS (ERR-T) These errors can be combined to give the C2296 9 7 following average total errors. C2296 9 8 (ERR-1,1.,5.) integrated beam intensity. C2296 9 9 (ERR-2) electroplated target density. C2296 9 10 (ERR-3,20.,25.) disintegration rates for negatron- C2296 9 11 emitting fission products, due mainly to counting C2296 9 12 correction uncertainties. C2296 9 13 STATUS (TABLE) Table I, page 438. C2296 9 14 ENDBIB 12 0 C2296 9 15 COMMON 2 3 C2296 9 16 ERR-T ERR-2 C2296 9 17 PER-CENT PER-CENT C2296 9 18 25.0 10.0 C2296 9 19 ENDCOMMON 3 0 C2296 9 20 DATA 2 7 C2296 9 21 EN DATA C2296 9 22 MEV MB C2296 9 23 25.2 10.0 C2296 9 24 28.7 12.0 C2296 9 25 30.2 17.0 C2296 9 26 33.0 20.0 C2296 9 27 36.6 22.0 C2296 9 28 42.2 15.0 C2296 9 29 47.4 19.0 C2296 9 30 ENDDATA 9 0 C2296 9 31 ENDSUBENT 30 0 C2296 999999 SUBENT C2296010 20180511 C175C2296 10 1 BIB 4 12 C2296 10 2 REACTION (94-PU-238(A,F)58-CE-143,(CUM),SIG) C2296 10 3 SAMPLE (94-PU-238,ENR=0.938) C2296 10 4 (94-PU-239,ENR=0.058) and small amounts of C2296 10 5 Pu-240,Pu-241 and Pu-242. C2296 10 6 ERR-ANALYS (ERR-T) These errors can be combined to give the C2296 10 7 following average total errors. C2296 10 8 (ERR-1,1.,5.) integrated beam intensity. C2296 10 9 (ERR-2) electroplated target density. C2296 10 10 (ERR-3,20.,25.) disintegration rates for negatron- C2296 10 11 emitting fission products, due mainly to counting C2296 10 12 correction uncertainties. C2296 10 13 STATUS (TABLE) Table I, page 438. C2296 10 14 ENDBIB 12 0 C2296 10 15 COMMON 2 3 C2296 10 16 ERR-T ERR-2 C2296 10 17 PER-CENT PER-CENT C2296 10 18 25.0 10.0 C2296 10 19 ENDCOMMON 3 0 C2296 10 20 DATA 2 3 C2296 10 21 EN DATA C2296 10 22 MEV MB C2296 10 23 30.2 25.0 C2296 10 24 36.6 34.0 C2296 10 25 42.2 22.0 C2296 10 26 ENDDATA 5 0 C2296 10 27 ENDSUBENT 26 0 C2296 1099999 SUBENT C2296011 20180511 C175C2296 11 1 BIB 4 12 C2296 11 2 REACTION (94-PU-238(A,F)60-ND-147,(CUM),SIG) C2296 11 3 SAMPLE (94-PU-238,ENR=0.938) C2296 11 4 (94-PU-239,ENR=0.058) and small amounts of C2296 11 5 Pu-240,Pu-241 and Pu-242. C2296 11 6 ERR-ANALYS (ERR-T) These errors can be combined to give the C2296 11 7 following average total errors. C2296 11 8 (ERR-1,1.,5.) integrated beam intensity. C2296 11 9 (ERR-2) electroplated target density. C2296 11 10 (ERR-3,20.,25.) disintegration rates for negatron- C2296 11 11 emitting fission products, due mainly to counting C2296 11 12 correction uncertainties. C2296 11 13 STATUS (TABLE) Table I, page 438. C2296 11 14 ENDBIB 12 0 C2296 11 15 COMMON 2 3 C2296 11 16 ERR-T ERR-2 C2296 11 17 PER-CENT PER-CENT C2296 11 18 25.0 10.0 C2296 11 19 ENDCOMMON 3 0 C2296 11 20 DATA 2 3 C2296 11 21 EN DATA C2296 11 22 MEV MB C2296 11 23 30.2 17.0 C2296 11 24 36.6 23.0 C2296 11 25 42.2 20.0 C2296 11 26 ENDDATA 5 0 C2296 11 27 ENDSUBENT 26 0 C2296 1199999 SUBENT C2296012 20180511 C175C2296 12 1 BIB 4 12 C2296 12 2 REACTION (94-PU-238(A,F)63-EU-156,(CUM),SIG) C2296 12 3 SAMPLE (94-PU-238,ENR=0.938) C2296 12 4 (94-PU-239,ENR=0.058) and small amounts of C2296 12 5 Pu-240,Pu-241 and Pu-242. C2296 12 6 ERR-ANALYS (ERR-T) These errors can be combined to give the C2296 12 7 following average total errors. C2296 12 8 (ERR-1,1.,5.) integrated beam intensity. C2296 12 9 (ERR-2) electroplated target density. C2296 12 10 (ERR-3,20.,25.) disintegration rates for negatron- C2296 12 11 emitting fission products, due mainly to counting C2296 12 12 correction uncertainties. C2296 12 13 STATUS (TABLE) Table I, page 438. C2296 12 14 ENDBIB 12 0 C2296 12 15 COMMON 2 3 C2296 12 16 ERR-T ERR-2 C2296 12 17 PER-CENT PER-CENT C2296 12 18 25.0 10.0 C2296 12 19 ENDCOMMON 3 0 C2296 12 20 DATA 2 3 C2296 12 21 EN DATA C2296 12 22 MEV MB C2296 12 23 30.2 2.8 C2296 12 24 36.6 3.6 C2296 12 25 42.2 3.7 C2296 12 26 ENDDATA 5 0 C2296 12 27 ENDSUBENT 26 0 C2296 1299999 SUBENT C2296013 20180511 C175C2296 13 1 BIB 4 12 C2296 13 2 REACTION (94-PU-238(A,F)65-TB-161,(CUM),SIG) C2296 13 3 SAMPLE (94-PU-238,ENR=0.938) C2296 13 4 (94-PU-239,ENR=0.058) and small amounts of C2296 13 5 Pu-240,Pu-241 and Pu-242. C2296 13 6 ERR-ANALYS (ERR-T) These errors can be combined to give the C2296 13 7 following average total errors. C2296 13 8 (ERR-1,1.,5.) integrated beam intensity. C2296 13 9 (ERR-2) electroplated target density. C2296 13 10 (ERR-3,20.,25.) disintegration rates for negatron- C2296 13 11 emitting fission products, due mainly to counting C2296 13 12 correction uncertainties. C2296 13 13 STATUS (TABLE) Table I, page 438. C2296 13 14 ENDBIB 12 0 C2296 13 15 COMMON 2 3 C2296 13 16 ERR-T ERR-2 C2296 13 17 PER-CENT PER-CENT C2296 13 18 25.0 10.0 C2296 13 19 ENDCOMMON 3 0 C2296 13 20 DATA 2 3 C2296 13 21 EN DATA C2296 13 22 MEV MB C2296 13 23 30.2 0.48 C2296 13 24 36.6 1.9 C2296 13 25 42.2 1.0 C2296 13 26 ENDDATA 5 0 C2296 13 27 ENDSUBENT 26 0 C2296 1399999 SUBENT C2296014 20180511 C175C2296 14 1 BIB 6 14 C2296 14 2 REACTION (94-PU-239(A,N)96-CM-242,,SIG) C2296 14 3 SAMPLE (94-PU-239,ENR=0.99) C2296 14 4 ERR-ANALYS (ERR-T) These errors can be combined to give the C2296 14 5 following average total errors. C2296 14 6 (ERR-1,1.,5.) integrated beam intensity. C2296 14 7 (ERR-2) electroplated target density. C2296 14 8 (ERR-3) disintegration rates for alpha particle- C2296 14 9 emitting spallation products. C2296 14 10 FLAG (1.) Value thus indicated has been adjusted to the C2296 14 11 (alpha,n) excitation function and serves as a basis C2296 14 12 for estimating all other cross sections, otherwise C2296 14 13 only of relative significance, at this energy. C2296 14 14 DECAY-DATA (96-CM-242,162.0D,A) C2296 14 15 STATUS (TABLE) Table II, page 439. C2296 14 16 ENDBIB 14 0 C2296 14 17 COMMON 3 3 C2296 14 18 ERR-T ERR-2 ERR-3 C2296 14 19 PER-CENT PER-CENT PER-CENT C2296 14 20 15.0 10.0 10.0 C2296 14 21 ENDCOMMON 3 0 C2296 14 22 DATA 3 12 C2296 14 23 EN DATA FLAG C2296 14 24 MEV MB NO-DIM C2296 14 25 20.2 1.1 C2296 14 26 24.5 0.84 C2296 14 27 26.8 1.1 1. C2296 14 28 27.5 1.3 C2296 14 29 34.0 2.4 C2296 14 30 38.0 2.2 C2296 14 31 39.2 1.8 C2296 14 32 40.7 0.97 C2296 14 33 43.8 1.5 1. C2296 14 34 44.3 1.6 1. C2296 14 35 46.0 2.6 C2296 14 36 47.5 0.82 C2296 14 37 ENDDATA 14 0 C2296 14 38 ENDSUBENT 37 0 C2296 1499999 SUBENT C2296015 20180511 C175C2296 15 1 BIB 5 11 C2296 15 2 REACTION (94-PU-239(A,2N)96-CM-241,,SIG) C2296 15 3 SAMPLE (94-PU-239,ENR=0.99) C2296 15 4 ERR-ANALYS (ERR-T) These errors can be combined to give the C2296 15 5 following average total errors. C2296 15 6 (ERR-1,1.,5.) integrated beam intensity. C2296 15 7 (ERR-2) electroplated target density. C2296 15 8 (ERR-3,20.,25.) disintegration rates for electron- C2296 15 9 capture-unstable products, due mainly to counting C2296 15 10 efficiency uncertainties. C2296 15 11 DECAY-DATA (96-CM-241,35.0D,EC) C2296 15 12 STATUS (TABLE) Table II, page 439. C2296 15 13 ENDBIB 11 0 C2296 15 14 COMMON 2 3 C2296 15 15 ERR-T ERR-2 C2296 15 16 PER-CENT PER-CENT C2296 15 17 25.0 10.0 C2296 15 18 ENDCOMMON 3 0 C2296 15 19 DATA 2 11 C2296 15 20 EN DATA C2296 15 21 MEV MB C2296 15 22 24.5 6.7 C2296 15 23 26.8 9.8 C2296 15 24 27.5 12.0 C2296 15 25 34.0 9.5 C2296 15 26 38.0 9.0 C2296 15 27 39.2 8.1 C2296 15 28 40.7 7.3 C2296 15 29 43.8 7.5 C2296 15 30 44.3 5.8 C2296 15 31 46.0 4.2 C2296 15 32 47.5 4.6 C2296 15 33 ENDDATA 13 0 C2296 15 34 ENDSUBENT 33 0 C2296 1599999 SUBENT C2296016 20180511 C175C2296 16 1 BIB 5 10 C2296 16 2 REACTION (94-PU-239(A,3N)96-CM-240,,SIG) C2296 16 3 SAMPLE (94-PU-239,ENR=0.99) C2296 16 4 ERR-ANALYS (ERR-T) These errors can be combined to give the C2296 16 5 following average total errors. C2296 16 6 (ERR-1,1.,5.) integrated beam intensity. C2296 16 7 (ERR-2) electroplated target density. C2296 16 8 (ERR-3) disintegration rates for alpha particle- C2296 16 9 emitting spallation products. C2296 16 10 DECAY-DATA (96-CM-240,27.0D,A) C2296 16 11 STATUS (TABLE) Table II, page 439. C2296 16 12 ENDBIB 10 0 C2296 16 13 COMMON 3 3 C2296 16 14 ERR-T ERR-2 ERR-3 C2296 16 15 PER-CENT PER-CENT PER-CENT C2296 16 16 15.0 10.0 10.0 C2296 16 17 ENDCOMMON 3 0 C2296 16 18 DATA 2 11 C2296 16 19 EN DATA C2296 16 20 MEV MB C2296 16 21 24.5 0.00001 C2296 16 22 26.8 1.2 C2296 16 23 27.5 0.86 C2296 16 24 34.0 3.5 C2296 16 25 38.0 4.5 C2296 16 26 39.2 3.6 C2296 16 27 40.7 2.3 C2296 16 28 43.8 2.7 C2296 16 29 44.3 3.0 C2296 16 30 46.0 2.1 C2296 16 31 47.5 1.9 C2296 16 32 ENDDATA 13 0 C2296 16 33 ENDSUBENT 32 0 C2296 1699999 SUBENT C2296017 20180511 C175C2296 17 1 BIB 5 11 C2296 17 2 REACTION (94-PU-239(A,4N)96-CM-239,,SIG) C2296 17 3 SAMPLE (94-PU-239,ENR=0.99) C2296 17 4 ERR-ANALYS (ERR-T) These errors can be combined to give the C2296 17 5 following average total errors. C2296 17 6 (ERR-1,1.,5.) integrated beam intensity. C2296 17 7 (ERR-2) electroplated target density. C2296 17 8 (ERR-3,20.,25.) disintegration rates for electron- C2296 17 9 capture-unstable products, due mainly to counting C2296 17 10 efficiency uncertainties. C2296 17 11 DECAY-DATA (96-CM-239,3.0HR,EC) C2296 17 12 STATUS (TABLE) Table II, page 439. C2296 17 13 ENDBIB 11 0 C2296 17 14 COMMON 2 3 C2296 17 15 ERR-T ERR-2 C2296 17 16 PER-CENT PER-CENT C2296 17 17 25.0 10.0 C2296 17 18 ENDCOMMON 3 0 C2296 17 19 DATA 2 2 C2296 17 20 EN DATA C2296 17 21 MEV MB C2296 17 22 40.7 0.8 C2296 17 23 47.5 0.6 C2296 17 24 ENDDATA 4 0 C2296 17 25 ENDSUBENT 24 0 C2296 1799999 SUBENT C2296018 20241031 C243C229601800001 BIB 6 12 C229601800002 REACTION (94-PU-239(A,5N)96-CM-238,,SIG) C229601800003 SAMPLE (94-PU-239,ENR=0.99) C229601800004 ERR-ANALYS (ERR-T) These errors can be combined to give the C229601800005 following average total errors. C229601800006 (ERR-1,1.,5.) integrated beam intensity. C229601800007 (ERR-2) electroplated target density. C229601800008 (ERR-3,20.,25.) disintegration rates for electron- C229601800009 capture-unstable products, due mainly to counting C229601800010 efficiency uncertainties. C229601800011 DECAY-DATA (96-CM-238,2.5HR,A,,0.018) C229601800012 STATUS (TABLE,,R.A.Glass+,J,PR,104,434,1956) Tab.II, p.439. C229601800013 HISTORY (20241028A) DECAY-DATA: Radiation field replaced C229601800014 ENDBIB 12 0 C229601800015 COMMON 2 3 C229601800016 ERR-T ERR-2 C229601800017 PER-CENT PER-CENT C229601800018 25.0 10.0 C229601800019 ENDCOMMON 3 0 C229601800020 DATA 2 1 C229601800021 EN DATA C229601800022 MEV MB C229601800023 46.0 0.004 C229601800024 ENDDATA 3 0 C229601800025 ENDSUBENT 24 0 C229601899999 SUBENT C2296019 20180511 C175C2296 19 1 BIB 5 13 C2296 19 2 REACTION (94-PU-239(A,P)95-AM-242-G,,SIG) C2296 19 3 SAMPLE (94-PU-239,ENR=0.99) C2296 19 4 ERR-ANALYS (ERR-T) These errors can be combined to give the C2296 19 5 following average total errors. C2296 19 6 (ERR-1,1.,5.) integrated beam intensity. C2296 19 7 (ERR-2) electroplated target density. C2296 19 8 (ERR-3,20.,25.) disintegration rates for electron- C2296 19 9 capture-unstable products, due mainly to counting C2296 19 10 efficiency uncertainties. C2296 19 11 DECAY-DATA (95-AM-242-G,16.0HR,B-) C2296 19 12 Note by compiler: The 16hr Am242 activity is designatedC2296 19 13 by authors as Am242m. C2296 19 14 STATUS (TABLE) Table II, page 439. C2296 19 15 ENDBIB 13 0 C2296 19 16 COMMON 2 3 C2296 19 17 ERR-T ERR-2 C2296 19 18 PER-CENT PER-CENT C2296 19 19 25.0 10.0 C2296 19 20 ENDCOMMON 3 0 C2296 19 21 DATA 2 9 C2296 19 22 EN DATA C2296 19 23 MEV MB C2296 19 24 20.2 0.030 C2296 19 25 24.5 0.58 C2296 19 26 26.8 0.72 C2296 19 27 27.5 0.29 C2296 19 28 34.0 1.3 C2296 19 29 38.0 0.96 C2296 19 30 39.2 0.58 C2296 19 31 40.7 1.1 C2296 19 32 47.5 0.56 C2296 19 33 ENDDATA 11 0 C2296 19 34 ENDSUBENT 33 0 C2296 1999999 SUBENT C2296020 20180511 C175C2296 20 1 BIB 5 11 C2296 20 2 REACTION (94-PU-239(A,X)95-AM-240,,SIG) C2296 20 3 SAMPLE (94-PU-239,ENR=0.99) C2296 20 4 ERR-ANALYS (ERR-T) These errors can be combined to give the C2296 20 5 following average total errors. C2296 20 6 (ERR-1,1.,5.) integrated beam intensity. C2296 20 7 (ERR-2) electroplated target density. C2296 20 8 (ERR-3,20.,25.) disintegration rates for electron- C2296 20 9 capture-unstable products, due mainly to counting C2296 20 10 efficiency uncertainties. C2296 20 11 DECAY-DATA (95-AM-240,51.0HR,EC) C2296 20 12 STATUS (TABLE) Table II, page 439. C2296 20 13 ENDBIB 11 0 C2296 20 14 COMMON 2 3 C2296 20 15 ERR-T ERR-2 C2296 20 16 PER-CENT PER-CENT C2296 20 17 25.0 10.0 C2296 20 18 ENDCOMMON 3 0 C2296 20 19 DATA 2 8 C2296 20 20 EN DATA C2296 20 21 MEV MB C2296 20 22 26.8 0.30 C2296 20 23 34.0 5.2 C2296 20 24 38.0 7.7 C2296 20 25 39.2 9.6 C2296 20 26 40.7 1.4 C2296 20 27 43.8 15.0 C2296 20 28 46.0 13.0 C2296 20 29 47.5 17.0 C2296 20 30 ENDDATA 10 0 C2296 20 31 ENDSUBENT 30 0 C2296 2099999 SUBENT C2296021 20180511 C175C2296 21 1 BIB 5 11 C2296 21 2 REACTION (94-PU-239(A,X)95-AM-239,,SIG) C2296 21 3 SAMPLE (94-PU-239,ENR=0.99) C2296 21 4 ERR-ANALYS (ERR-T) These errors can be combined to give the C2296 21 5 following average total errors. C2296 21 6 (ERR-1,1.,5.) integrated beam intensity. C2296 21 7 (ERR-2) electroplated target density. C2296 21 8 (ERR-3,20.,25.) disintegration rates for electron- C2296 21 9 capture-unstable products, due mainly to counting C2296 21 10 efficiency uncertainties. C2296 21 11 DECAY-DATA (95-AM-239,12.0HR,EC) C2296 21 12 STATUS (TABLE) Table II, page 439. C2296 21 13 ENDBIB 11 0 C2296 21 14 COMMON 2 3 C2296 21 15 ERR-T ERR-2 C2296 21 16 PER-CENT PER-CENT C2296 21 17 25.0 10.0 C2296 21 18 ENDCOMMON 3 0 C2296 21 19 DATA 2 4 C2296 21 20 EN DATA-MAX C2296 21 21 MEV MB C2296 21 22 38.0 0.3 C2296 21 23 39.2 0.4 C2296 21 24 46.0 0.4 C2296 21 25 47.5 0.3 C2296 21 26 ENDDATA 6 0 C2296 21 27 ENDSUBENT 26 0 C2296 2199999 SUBENT C2296022 20180514 C175C2296 22 1 BIB 5 11 C2296 22 2 REACTION (94-PU-239(A,F)35-BR-82,,SIG) C2296 22 3 SAMPLE (94-PU-239,ENR=0.99) C2296 22 4 ERR-ANALYS (ERR-T) These errors can be combined to give the C2296 22 5 following average total errors. C2296 22 6 (ERR-1,1.,5.) integrated beam intensity. C2296 22 7 (ERR-2) electroplated target density. C2296 22 8 (ERR-3,20.,25.) disintegration rates for negatron- C2296 22 9 emitting fission products, due mainly to counting C2296 22 10 correction uncertainties. C2296 22 11 FLAG (1.) Product is a shielded nuclide. C2296 22 12 STATUS (TABLE) Table II, page 439. C2296 22 13 ENDBIB 11 0 C2296 22 14 COMMON 2 3 C2296 22 15 ERR-T ERR-2 C2296 22 16 PER-CENT PER-CENT C2296 22 17 25.0 10.0 C2296 22 18 ENDCOMMON 3 0 C2296 22 19 DATA 3 1 C2296 22 20 EN DATA FLAG C2296 22 21 MEV MB NO-DIM C2296 22 22 24.0 0.5 1. C2296 22 23 ENDDATA 3 0 C2296 22 24 ENDSUBENT 23 0 C2296 2299999 SUBENT C2296023 20180514 C175C2296 23 1 BIB 4 10 C2296 23 2 REACTION (94-PU-239(A,F)35-BR-83,(CUM),SIG) C2296 23 3 SAMPLE (94-PU-239,ENR=0.99) C2296 23 4 ERR-ANALYS (ERR-T) These errors can be combined to give the C2296 23 5 following average total errors. C2296 23 6 (ERR-1,1.,5.) integrated beam intensity. C2296 23 7 (ERR-2) electroplated target density. C2296 23 8 (ERR-3,20.,25.) disintegration rates for negatron- C2296 23 9 emitting fission products, due mainly to counting C2296 23 10 correction uncertainties. C2296 23 11 STATUS (TABLE) Table II, page 439. C2296 23 12 ENDBIB 10 0 C2296 23 13 COMMON 2 3 C2296 23 14 ERR-T ERR-2 C2296 23 15 PER-CENT PER-CENT C2296 23 16 25.0 10.0 C2296 23 17 ENDCOMMON 3 0 C2296 23 18 DATA 2 1 C2296 23 19 EN DATA C2296 23 20 MEV MB C2296 23 21 24.0 0.23 C2296 23 22 ENDDATA 3 0 C2296 23 23 ENDSUBENT 22 0 C2296 2399999 SUBENT C2296024 20180514 C175C2296 24 1 BIB 5 12 C2296 24 2 REACTION (94-PU-239(A,F)38-SR-89,(CUM),SIG) C2296 24 3 SAMPLE (94-PU-239,ENR=0.99) C2296 24 4 ERR-ANALYS (ERR-T) These errors can be combined to give the C2296 24 5 following average total errors. C2296 24 6 (ERR-1,1.,5.) integrated beam intensity. C2296 24 7 (ERR-2) electroplated target density. C2296 24 8 (ERR-3,20.,25.) disintegration rates for negatron- C2296 24 9 emitting fission products, due mainly to counting C2296 24 10 correction uncertainties. C2296 24 11 FLAG (1.) Value indicated is an average of two C2296 24 12 determinations. C2296 24 13 STATUS (TABLE) Table II, page 439. C2296 24 14 ENDBIB 12 0 C2296 24 15 COMMON 2 3 C2296 24 16 ERR-T ERR-2 C2296 24 17 PER-CENT PER-CENT C2296 24 18 25.0 10.0 C2296 24 19 ENDCOMMON 3 0 C2296 24 20 DATA 3 10 C2296 24 21 EN DATA FLAG C2296 24 22 MEV MB NO-DIM C2296 24 23 20.2 0.06 C2296 24 24 24.0 0.95 C2296 24 25 24.5 2.0 C2296 24 26 27.5 3.4 C2296 24 27 34.0 4.3 C2296 24 28 38.0 15.0 1. C2296 24 29 40.7 9.5 C2296 24 30 43.8 16.0 C2296 24 31 46.0 14.0 C2296 24 32 47.5 15.0 C2296 24 33 ENDDATA 12 0 C2296 24 34 ENDSUBENT 33 0 C2296 2499999 SUBENT C2296025 20180514 C175C2296 25 1 BIB 5 12 C2296 25 2 REACTION (94-PU-239(A,F)38-SR-91,(CUM),SIG) C2296 25 3 SAMPLE (94-PU-239,ENR=0.99) C2296 25 4 ERR-ANALYS (ERR-T) These errors can be combined to give the C2296 25 5 following average total errors. C2296 25 6 (ERR-1,1.,5.) integrated beam intensity. C2296 25 7 (ERR-2) electroplated target density. C2296 25 8 (ERR-3,20.,25.) disintegration rates for negatron- C2296 25 9 emitting fission products, due mainly to counting C2296 25 10 correction uncertainties. C2296 25 11 FLAG (1.) Value indicated is an average of two C2296 25 12 determinations. C2296 25 13 STATUS (TABLE) Table II, page 439. C2296 25 14 ENDBIB 12 0 C2296 25 15 COMMON 2 3 C2296 25 16 ERR-T ERR-2 C2296 25 17 PER-CENT PER-CENT C2296 25 18 25.0 10.0 C2296 25 19 ENDCOMMON 3 0 C2296 25 20 DATA 3 9 C2296 25 21 EN DATA FLAG C2296 25 22 MEV MB NO-DIM C2296 25 23 20.2 0.11 C2296 25 24 24.0 2.1 C2296 25 25 24.5 3.5 C2296 25 26 34.0 5.4 C2296 25 27 38.0 14.0 1. C2296 25 28 40.7 15.0 C2296 25 29 43.8 26.0 C2296 25 30 46.0 17.0 C2296 25 31 47.5 34.0 C2296 25 32 ENDDATA 11 0 C2296 25 33 ENDSUBENT 32 0 C2296 2599999 SUBENT C2296026 20180514 C175C2296 26 1 BIB 4 10 C2296 26 2 REACTION (94-PU-239(A,F)38-SR-92,(CUM),SIG) C2296 26 3 SAMPLE (94-PU-239,ENR=0.99) C2296 26 4 ERR-ANALYS (ERR-T) These errors can be combined to give the C2296 26 5 following average total errors. C2296 26 6 (ERR-1,1.,5.) integrated beam intensity. C2296 26 7 (ERR-2) electroplated target density. C2296 26 8 (ERR-3,20.,25.) disintegration rates for negatron- C2296 26 9 emitting fission products, due mainly to counting C2296 26 10 correction uncertainties. C2296 26 11 STATUS (TABLE) Table II, page 439. C2296 26 12 ENDBIB 10 0 C2296 26 13 COMMON 2 3 C2296 26 14 ERR-T ERR-2 C2296 26 15 PER-CENT PER-CENT C2296 26 16 25.0 10.0 C2296 26 17 ENDCOMMON 3 0 C2296 26 18 DATA 2 7 C2296 26 19 EN DATA C2296 26 20 MEV MB C2296 26 21 20.2 0.13 C2296 26 22 24.0 1.4 C2296 26 23 34.0 6.2 C2296 26 24 38.0 13.0 C2296 26 25 40.7 13.0 C2296 26 26 46.0 17.0 C2296 26 27 47.5 21.0 C2296 26 28 ENDDATA 9 0 C2296 26 29 ENDSUBENT 28 0 C2296 2699999 SUBENT C2296027 20180514 C175C2296 27 1 BIB 4 10 C2296 27 2 REACTION (94-PU-239(A,F)44-RU-105,(CUM),SIG) C2296 27 3 SAMPLE (94-PU-239,ENR=0.99) C2296 27 4 ERR-ANALYS (ERR-T) These errors can be combined to give the C2296 27 5 following average total errors. C2296 27 6 (ERR-1,1.,5.) integrated beam intensity. C2296 27 7 (ERR-2) electroplated target density. C2296 27 8 (ERR-3,20.,25.) disintegration rates for negatron- C2296 27 9 emitting fission products, due mainly to counting C2296 27 10 correction uncertainties. C2296 27 11 STATUS (TABLE) Table II, page 439. C2296 27 12 ENDBIB 10 0 C2296 27 13 COMMON 2 3 C2296 27 14 ERR-T ERR-2 C2296 27 15 PER-CENT PER-CENT C2296 27 16 25.0 10.0 C2296 27 17 ENDCOMMON 3 0 C2296 27 18 DATA 2 1 C2296 27 19 EN DATA C2296 27 20 MEV MB C2296 27 21 34.0 8.6 C2296 27 22 ENDDATA 3 0 C2296 27 23 ENDSUBENT 22 0 C2296 2799999 SUBENT C2296028 20180514 C175C2296 28 1 BIB 5 12 C2296 28 2 REACTION (94-PU-239(A,F)48-CD-115,(CUM),SIG) M+G C2296 28 3 SAMPLE (94-PU-239,ENR=0.99) C2296 28 4 ERR-ANALYS (ERR-T) These errors can be combined to give the C2296 28 5 following average total errors. C2296 28 6 (ERR-1,1.,5.) integrated beam intensity. C2296 28 7 (ERR-2) electroplated target density. C2296 28 8 (ERR-3,20.,25.) disintegration rates for negatron- C2296 28 9 emitting fission products, due mainly to counting C2296 28 10 correction uncertainties. C2296 28 11 FLAG (1.) Value interpolated from graph of peak-to-valley C2296 28 12 ratio of yield curves vs energy. C2296 28 13 STATUS (TABLE) Table II, page 439. C2296 28 14 ENDBIB 12 0 C2296 28 15 COMMON 2 3 C2296 28 16 ERR-T ERR-2 C2296 28 17 PER-CENT PER-CENT C2296 28 18 25.0 10.0 C2296 28 19 ENDCOMMON 3 0 C2296 28 20 DATA 3 9 C2296 28 21 EN DATA FLAG C2296 28 22 MEV MB NO-DIM C2296 28 23 20.2 0.048 C2296 28 24 24.0 0.7 1. C2296 28 25 24.5 1.4 C2296 28 26 27.5 2.6 C2296 28 27 34.0 5.3 C2296 28 28 38.0 9.0 C2296 28 29 40.7 38.0 C2296 28 30 43.8 68.0 C2296 28 31 46.0 55.0 C2296 28 32 ENDDATA 11 0 C2296 28 33 ENDSUBENT 32 0 C2296 2899999 SUBENT C2296029 20180514 C175C2296 29 1 BIB 4 10 C2296 29 2 REACTION (94-PU-239(A,F)48-CD-117,(CUM),SIG) C2296 29 3 SAMPLE (94-PU-239,ENR=0.99) C2296 29 4 ERR-ANALYS (ERR-T) These errors can be combined to give the C2296 29 5 following average total errors. C2296 29 6 (ERR-1,1.,5.) integrated beam intensity. C2296 29 7 (ERR-2) electroplated target density. C2296 29 8 (ERR-3,20.,25.) disintegration rates for negatron- C2296 29 9 emitting fission products, due mainly to counting C2296 29 10 correction uncertainties. C2296 29 11 STATUS (TABLE) Table II, page 439. C2296 29 12 ENDBIB 10 0 C2296 29 13 COMMON 2 3 C2296 29 14 ERR-T ERR-2 C2296 29 15 PER-CENT PER-CENT C2296 29 16 25.0 10.0 C2296 29 17 ENDCOMMON 3 0 C2296 29 18 DATA 2 6 C2296 29 19 EN DATA C2296 29 20 MEV MB C2296 29 21 20.2 0.04 C2296 29 22 34.0 6.2 C2296 29 23 38.0 18.0 C2296 29 24 40.7 23.0 C2296 29 25 46.0 48.0 C2296 29 26 47.5 85.0 C2296 29 27 ENDDATA 8 0 C2296 29 28 ENDSUBENT 27 0 C2296 2999999 SUBENT C2296030 20180514 C175C2296 30 1 BIB 4 10 C2296 30 2 REACTION (94-PU-239(A,F)53-I-131,(CUM),SIG) C2296 30 3 SAMPLE (94-PU-239,ENR=0.99) C2296 30 4 ERR-ANALYS (ERR-T) These errors can be combined to give the C2296 30 5 following average total errors. C2296 30 6 (ERR-1,1.,5.) integrated beam intensity. C2296 30 7 (ERR-2) electroplated target density. C2296 30 8 (ERR-3,20.,25.) disintegration rates for negatron- C2296 30 9 emitting fission products, due mainly to counting C2296 30 10 correction uncertainties. C2296 30 11 STATUS (TABLE) Table II, page 439. C2296 30 12 ENDBIB 10 0 C2296 30 13 COMMON 2 3 C2296 30 14 ERR-T ERR-2 C2296 30 15 PER-CENT PER-CENT C2296 30 16 25.0 10.0 C2296 30 17 ENDCOMMON 3 0 C2296 30 18 DATA 2 1 C2296 30 19 EN DATA C2296 30 20 MEV MB C2296 30 21 24.0 1.6 C2296 30 22 ENDDATA 3 0 C2296 30 23 ENDSUBENT 22 0 C2296 3099999 SUBENT C2296031 20180514 C175C2296 31 1 BIB 4 10 C2296 31 2 REACTION (94-PU-239(A,F)53-I-133,(CUM),SIG) C2296 31 3 SAMPLE (94-PU-239,ENR=0.99) C2296 31 4 ERR-ANALYS (ERR-T) These errors can be combined to give the C2296 31 5 following average total errors. C2296 31 6 (ERR-1,1.,5.) integrated beam intensity. C2296 31 7 (ERR-2) electroplated target density. C2296 31 8 (ERR-3,20.,25.) disintegration rates for negatron- C2296 31 9 emitting fission products, due mainly to counting C2296 31 10 correction uncertainties. C2296 31 11 STATUS (TABLE) Table II, page 439. C2296 31 12 ENDBIB 10 0 C2296 31 13 COMMON 2 3 C2296 31 14 ERR-T ERR-2 C2296 31 15 PER-CENT PER-CENT C2296 31 16 25.0 10.0 C2296 31 17 ENDCOMMON 3 0 C2296 31 18 DATA 2 1 C2296 31 19 EN DATA C2296 31 20 MEV MB C2296 31 21 24.0 2.1 C2296 31 22 ENDDATA 3 0 C2296 31 23 ENDSUBENT 22 0 C2296 3199999 SUBENT C2296032 20180514 C175C2296 32 1 BIB 4 10 C2296 32 2 REACTION (94-PU-239(A,F)56-BA-139,(CUM),SIG) C2296 32 3 SAMPLE (94-PU-239,ENR=0.99) C2296 32 4 ERR-ANALYS (ERR-T) These errors can be combined to give the C2296 32 5 following average total errors. C2296 32 6 (ERR-1,1.,5.) integrated beam intensity. C2296 32 7 (ERR-2) electroplated target density. C2296 32 8 (ERR-3,20.,25.) disintegration rates for negatron- C2296 32 9 emitting fission products, due mainly to counting C2296 32 10 correction uncertainties. C2296 32 11 STATUS (TABLE) Table II, page 439. C2296 32 12 ENDBIB 10 0 C2296 32 13 COMMON 2 3 C2296 32 14 ERR-T ERR-2 C2296 32 15 PER-CENT PER-CENT C2296 32 16 25.0 10.0 C2296 32 17 ENDCOMMON 3 0 C2296 32 18 DATA 2 6 C2296 32 19 EN DATA C2296 32 20 MEV MB C2296 32 21 20.2 0.29 C2296 32 22 24.5 5.4 C2296 32 23 27.5 5.7 C2296 32 24 40.7 16.0 C2296 32 25 46.0 20.0 C2296 32 26 47.5 21.0 C2296 32 27 ENDDATA 8 0 C2296 32 28 ENDSUBENT 27 0 C2296 3299999 SUBENT C2296033 20180514 C175C2296 33 1 BIB 5 12 C2296 33 2 REACTION (94-PU-239(A,F)56-BA-140,(CUM),SIG) C2296 33 3 SAMPLE (94-PU-239,ENR=0.99) C2296 33 4 ERR-ANALYS (ERR-T) These errors can be combined to give the C2296 33 5 following average total errors. C2296 33 6 (ERR-1,1.,5.) integrated beam intensity. C2296 33 7 (ERR-2) electroplated target density. C2296 33 8 (ERR-3,20.,25.) disintegration rates for negatron- C2296 33 9 emitting fission products, due mainly to counting C2296 33 10 correction uncertainties. C2296 33 11 FLAG (1.) Value indicated is an average of two C2296 33 12 determinations. C2296 33 13 STATUS (TABLE) Table II, page 439. C2296 33 14 ENDBIB 12 0 C2296 33 15 COMMON 2 3 C2296 33 16 ERR-T ERR-2 C2296 33 17 PER-CENT PER-CENT C2296 33 18 25.0 10.0 C2296 33 19 ENDCOMMON 3 0 C2296 33 20 DATA 3 10 C2296 33 21 EN DATA FLAG C2296 33 22 MEV MB NO-DIM C2296 33 23 20.2 0.19 C2296 33 24 24.0 3.1 C2296 33 25 24.5 4.5 C2296 33 26 27.5 6.3 C2296 33 27 34.0 12.0 1. C2296 33 28 38.0 16.0 1. C2296 33 29 40.7 9.5 C2296 33 30 43.8 19.0 C2296 33 31 46.0 18.0 C2296 33 32 47.5 18.0 C2296 33 33 ENDDATA 12 0 C2296 33 34 ENDSUBENT 33 0 C2296 3399999 SUBENT C2296034 20180514 C175C2296 34 1 BIB 4 10 C2296 34 2 REACTION (94-PU-239(A,F)58-CE-143,(CUM),SIG) C2296 34 3 SAMPLE (94-PU-239,ENR=0.99) C2296 34 4 ERR-ANALYS (ERR-T) These errors can be combined to give the C2296 34 5 following average total errors. C2296 34 6 (ERR-1,1.,5.) integrated beam intensity. C2296 34 7 (ERR-2) electroplated target density. C2296 34 8 (ERR-3,20.,25.) disintegration rates for negatron- C2296 34 9 emitting fission products, due mainly to counting C2296 34 10 correction uncertainties. C2296 34 11 STATUS (TABLE) Table II, page 439. C2296 34 12 ENDBIB 10 0 C2296 34 13 COMMON 2 3 C2296 34 14 ERR-T ERR-2 C2296 34 15 PER-CENT PER-CENT C2296 34 16 25.0 10.0 C2296 34 17 ENDCOMMON 3 0 C2296 34 18 DATA 2 2 C2296 34 19 EN DATA C2296 34 20 MEV MB C2296 34 21 24.0 3.0 C2296 34 22 34.0 11.0 C2296 34 23 ENDDATA 4 0 C2296 34 24 ENDSUBENT 23 0 C2296 3499999 SUBENT C2296035 20180514 C175C2296 35 1 BIB 4 10 C2296 35 2 REACTION (94-PU-239(A,F)58-CE-145,(CUM),SIG) C2296 35 3 SAMPLE (94-PU-239,ENR=0.99) C2296 35 4 ERR-ANALYS (ERR-T) These errors can be combined to give the C2296 35 5 following average total errors. C2296 35 6 (ERR-1,1.,5.) integrated beam intensity. C2296 35 7 (ERR-2) electroplated target density. C2296 35 8 (ERR-3,20.,25.) disintegration rates for negatron- C2296 35 9 emitting fission products, due mainly to counting C2296 35 10 correction uncertainties. C2296 35 11 STATUS (TABLE) Table II, page 439. C2296 35 12 ENDBIB 10 0 C2296 35 13 COMMON 2 3 C2296 35 14 ERR-T ERR-2 C2296 35 15 PER-CENT PER-CENT C2296 35 16 25.0 10.0 C2296 35 17 ENDCOMMON 3 0 C2296 35 18 DATA 2 1 C2296 35 19 EN DATA C2296 35 20 MEV MB C2296 35 21 34.0 14.0 C2296 35 22 ENDDATA 3 0 C2296 35 23 ENDSUBENT 22 0 C2296 3599999 SUBENT C2296036 20180514 C175C2296 36 1 BIB 4 10 C2296 36 2 REACTION (94-PU-239(A,F)60-ND-147,(CUM),SIG) C2296 36 3 SAMPLE (94-PU-239,ENR=0.99) C2296 36 4 ERR-ANALYS (ERR-T) These errors can be combined to give the C2296 36 5 following average total errors. C2296 36 6 (ERR-1,1.,5.) integrated beam intensity. C2296 36 7 (ERR-2) electroplated target density. C2296 36 8 (ERR-3,20.,25.) disintegration rates for negatron- C2296 36 9 emitting fission products, due mainly to counting C2296 36 10 correction uncertainties. C2296 36 11 STATUS (TABLE) Table II, page 439. C2296 36 12 ENDBIB 10 0 C2296 36 13 COMMON 2 3 C2296 36 14 ERR-T ERR-2 C2296 36 15 PER-CENT PER-CENT C2296 36 16 25.0 10.0 C2296 36 17 ENDCOMMON 3 0 C2296 36 18 DATA 2 1 C2296 36 19 EN DATA C2296 36 20 MEV MB C2296 36 21 46.0 12.0 C2296 36 22 ENDDATA 3 0 C2296 36 23 ENDSUBENT 22 0 C2296 3699999 SUBENT C2296037 20180514 C175C2296 37 1 BIB 4 10 C2296 37 2 REACTION (94-PU-239(A,F)63-EU-156,(CUM),SIG) C2296 37 3 SAMPLE (94-PU-239,ENR=0.99) C2296 37 4 ERR-ANALYS (ERR-T) These errors can be combined to give the C2296 37 5 following average total errors. C2296 37 6 (ERR-1,1.,5.) integrated beam intensity. C2296 37 7 (ERR-2) electroplated target density. C2296 37 8 (ERR-3,20.,25.) disintegration rates for negatron- C2296 37 9 emitting fission products, due mainly to counting C2296 37 10 correction uncertainties. C2296 37 11 STATUS (TABLE) Table II, page 439. C2296 37 12 ENDBIB 10 0 C2296 37 13 COMMON 2 3 C2296 37 14 ERR-T ERR-2 C2296 37 15 PER-CENT PER-CENT C2296 37 16 25.0 10.0 C2296 37 17 ENDCOMMON 3 0 C2296 37 18 DATA 2 3 C2296 37 19 EN DATA C2296 37 20 MEV MB C2296 37 21 24.0 0.32 C2296 37 22 34.0 0.7 C2296 37 23 46.0 2.9 C2296 37 24 ENDDATA 5 0 C2296 37 25 ENDSUBENT 24 0 C2296 3799999 SUBENT C2296038 20180514 C175C2296 38 1 BIB 4 10 C2296 38 2 REACTION (94-PU-239(A,F)63-EU-157,(CUM),SIG) C2296 38 3 SAMPLE (94-PU-239,ENR=0.99) C2296 38 4 ERR-ANALYS (ERR-T) These errors can be combined to give the C2296 38 5 following average total errors. C2296 38 6 (ERR-1,1.,5.) integrated beam intensity. C2296 38 7 (ERR-2) electroplated target density. C2296 38 8 (ERR-3,20.,25.) disintegration rates for negatron- C2296 38 9 emitting fission products, due mainly to counting C2296 38 10 correction uncertainties. C2296 38 11 STATUS (TABLE) Table II, page 439. C2296 38 12 ENDBIB 10 0 C2296 38 13 COMMON 2 3 C2296 38 14 ERR-T ERR-2 C2296 38 15 PER-CENT PER-CENT C2296 38 16 25.0 10.0 C2296 38 17 ENDCOMMON 3 0 C2296 38 18 DATA 2 2 C2296 38 19 EN DATA C2296 38 20 MEV MB C2296 38 21 24.0 0.30 C2296 38 22 46.0 2.3 C2296 38 23 ENDDATA 4 0 C2296 38 24 ENDSUBENT 23 0 C2296 3899999 SUBENT C2296039 20180515 C175C2296 39 1 BIB 4 10 C2296 39 2 REACTION (94-PU-239(A,F)65-TB-161,(CUM),SIG) C2296 39 3 SAMPLE (94-PU-239,ENR=0.99) C2296 39 4 ERR-ANALYS (ERR-T) These errors can be combined to give the C2296 39 5 following average total errors. C2296 39 6 (ERR-1,1.,5.) integrated beam intensity. C2296 39 7 (ERR-2) electroplated target density. C2296 39 8 (ERR-3,20.,25.) disintegration rates for negatron- C2296 39 9 emitting fission products, due mainly to counting C2296 39 10 correction uncertainties. C2296 39 11 STATUS (TABLE) Table II, page 439. C2296 39 12 ENDBIB 10 0 C2296 39 13 COMMON 2 3 C2296 39 14 ERR-T ERR-2 C2296 39 15 PER-CENT PER-CENT C2296 39 16 25.0 10.0 C2296 39 17 ENDCOMMON 3 0 C2296 39 18 DATA 2 1 C2296 39 19 EN DATA C2296 39 20 MEV MB C2296 39 21 46.0 1.9 C2296 39 22 ENDDATA 3 0 C2296 39 23 ENDSUBENT 22 0 C2296 3999999 SUBENT C2296040 20180515 C175C2296 40 1 BIB 6 24 C2296 40 2 REACTION (94-PU-242(A,X)96-CM-244,CUM,SIG) C2296 40 3 Small contribution of (alpha,3n) reaction. C2296 40 4 SAMPLE (94-PU-242,ENR=0.378) C2296 40 5 (94-PU-238,ENR=0.586) C2296 40 6 (94-PU-239,ENR=0.034) and small amounts of Pu240 and C2296 40 7 Pu241. C2296 40 8 ERR-ANALYS (ERR-T) These errors can be combined to give the C2296 40 9 following average total errors. C2296 40 10 (ERR-1,1.,5.) integrated beam intensity. C2296 40 11 (ERR-2) electroplated target density. C2296 40 12 (ERR-3) disintegration rates for alpha particle- C2296 40 13 emitting spallation products. C2296 40 14 COMMENT -- Absolute cross sections were determined by C2296 40 15 referring relative cross sections to C2296 40 16 Pu238(alpha,2n)Cm240 reaction cross sections, since C2296 40 17 targets were 58.6% Pu238. C2296 40 18 -- Product and consequently cross section are for the C2296 40 19 sum of the (alpha,2n) and (alpha,pn) reaction. Cross C2296 40 20 sections also include small contributions from the C2296 40 21 (alpha,3n) reactions at the higher energies. C2296 40 22 -- Compiler's comment: corrected energy from 28.8 to C2296 40 23 38.8 MeV. C2296 40 24 MONITOR (94-PU-238(A,2N)96-CM-240,,SIG) C2296 40 25 STATUS (TABLE) Table III, page 439. C2296 40 26 ENDBIB 24 0 C2296 40 27 COMMON 3 3 C2296 40 28 ERR-T ERR-2 ERR-3 C2296 40 29 PER-CENT PER-CENT PER-CENT C2296 40 30 15.0 10.0 10.0 C2296 40 31 ENDCOMMON 3 0 C2296 40 32 DATA 2 7 C2296 40 33 EN DATA C2296 40 34 MEV MB C2296 40 35 23.6 103.0 C2296 40 36 25.9 116.0 C2296 40 37 27.1 70.0 C2296 40 38 28.5 68.0 C2296 40 39 32.8 30.0 C2296 40 40 38.8 24.0 C2296 40 41 43.5 35.0 C2296 40 42 ENDDATA 9 0 C2296 40 43 ENDSUBENT 42 0 C2296 4099999 SUBENT C2296041 20180515 C175C2296 41 1 BIB 7 20 C2296 41 2 REACTION (94-PU-242(A,4N)96-CM-242,,SIG) C2296 41 3 SAMPLE (94-PU-242,ENR=0.378) C2296 41 4 (94-PU-238,ENR=0.586) C2296 41 5 (94-PU-239,ENR=0.034) and small amounts of Pu240 and C2296 41 6 Pu241. C2296 41 7 ERR-ANALYS (ERR-T) These errors can be combined to give the C2296 41 8 following average total errors. C2296 41 9 (ERR-1,1.,5.) integrated beam intensity. C2296 41 10 (ERR-2) electroplated target density. C2296 41 11 (ERR-3) disintegration rates for alpha particle- C2296 41 12 emitting spallation products. C2296 41 13 DECAY-DATA (96-CM-242,162.0D,A) C2296 41 14 COMMENT -- Absolute cross sections were determined by referringC2296 41 15 relative cross sections to Pu238(alpha,2n)Cm240 C2296 41 16 reaction cross sections, since targets were 58.6% C2296 41 17 Pu238. C2296 41 18 -- Compiler's comment: corrected energy from 28.8 to C2296 41 19 38.8 MeV. C2296 41 20 MONITOR (94-PU-238(A,2N)96-CM-240,,SIG) C2296 41 21 STATUS (TABLE) Table III, page 439. C2296 41 22 ENDBIB 20 0 C2296 41 23 COMMON 3 3 C2296 41 24 ERR-T ERR-2 ERR-3 C2296 41 25 PER-CENT PER-CENT PER-CENT C2296 41 26 15.0 10.0 10.0 C2296 41 27 ENDCOMMON 3 0 C2296 41 28 DATA 2 3 C2296 41 29 EN DATA C2296 41 30 MEV MB C2296 41 31 32.8 1.8 C2296 41 32 38.8 8.8 C2296 41 33 43.5 8.3 C2296 41 34 ENDDATA 5 0 C2296 41 35 ENDSUBENT 34 0 C2296 4199999 SUBENT C2296042 20180515 C175C2296 42 1 BIB 6 15 C2296 42 2 REACTION (94-PU-238(A,N)96-CM-241,,SIG) C2296 42 3 SAMPLE (94-PU-238,ENR=0.938) C2296 42 4 (94-PU-239,ENR=0.058) and small amounts of C2296 42 5 Pu-240,Pu-241 and Pu-242. C2296 42 6 ERR-ANALYS (ERR-T) These errors can be combined to give the C2296 42 7 following average total errors. C2296 42 8 (ERR-1,1.,5.) integrated beam intensity. C2296 42 9 (ERR-2) electroplated target density. C2296 42 10 (ERR-3,20.,25.) disintegration rates for electron- C2296 42 11 capture-unstable products, due mainly to counting C2296 42 12 efficiency uncertainties. C2296 42 13 DECAY-DATA (96-CM-241,35.0D,EC) C2296 42 14 COMMENT -- Compiler's comment: corrected energy from 28.8 to C2296 42 15 38.8 MeV. C2296 42 16 STATUS (TABLE) Table III, page 439. C2296 42 17 ENDBIB 15 0 C2296 42 18 COMMON 2 3 C2296 42 19 ERR-T ERR-2 C2296 42 20 PER-CENT PER-CENT C2296 42 21 25.0 10.0 C2296 42 22 ENDCOMMON 3 0 C2296 42 23 DATA 2 7 C2296 42 24 EN DATA C2296 42 25 MEV MB C2296 42 26 23.6 6.8 C2296 42 27 25.9 8.2 C2296 42 28 27.1 6.5 C2296 42 29 28.5 7.8 C2296 42 30 32.8 6.2 C2296 42 31 38.8 2.9 C2296 42 32 43.5 2.8 C2296 42 33 ENDDATA 9 0 C2296 42 34 ENDSUBENT 33 0 C2296 4299999 ENDENTRY 42 0 C229699999999