ENTRY A0480 20231226 A105A0480 0 1 SUBENT A0480001 20231226 A105A0480 1 1 BIB 10 33 A0480 1 2 TITLE Spallation-fission competition in heaviest elements; A0480 1 3 Helium-ion-induced reactions in uranium isotopes A0480 1 4 AUTHOR (R.Vandenbosch,T.D.Thomas,S.E.Vandenbosch,R.A.Glass, A0480 1 5 G.T.Seaborg) A0480 1 6 INSTITUTE (1USABRK) A0480 1 7 REFERENCE (J,PR,111,1358,1958) A0480 1 8 (R,UCRL-3858,1957) -Additional data, experim. descript.A0480 1 9 FACILITY (CYCLO,1USABRK) A0480 1 10 METHOD (EDEG,SITA,BCINT,CHSEP,ACTIV,INTB,EXTB) A0480 1 11 DETECTOR (GEMUC) The disintegration rates were determined usingA0480 1 12 end window "Amperex" Geiger counter tubes A0480 1 13 (PROPC) The counting rates of spallation products whichA0480 1 14 decay by negatron emission or electron capture were A0480 1 15 determined with a methane-flow windowless proportional A0480 1 16 counter. A0480 1 17 (IOCH) The total disintegration rate of alpha-emitting A0480 1 18 samples was determined in a 52%-geometry argon-flow A0480 1 19 ionization chamber. A0480 1 20 REL-REF (M,,R.A.Glass+,J,PR,104,434,1956) - technical details A0480 1 21 COMMENT /By authors/ the counting rates of spallation products A0480 1 22 which decay by negatron emission or electron capture A0480 1 23 were determined with a methane-flow windowless A0480 1 24 proportional counter. A0480 1 25 HISTORY (19910207C) A0480 1 26 (19920429U) A0480 1 27 (19920207A) According to memo CP-D/123. A0480 1 28 (20160317A) SD:Updated to new date formats,lower case. A0480 1 29 BIB updated. REACTION code corrected in several A0480 1 30 Subents. SAMPLE moved to Subents 002-048. BIB updated A0480 1 31 in all Subents. A0480 1 32 (20200311A) SD: Corrections in all Subents. Subents A0480 1 33 022-030; 031-039; 040-048 merged. Subents 049-058 addedA0480 1 34 (20231226A) SD: Correction in Subent 040. A0480 1 35 ENDBIB 33 0 A0480 1 36 NOCOMMON 0 0 A0480 1 37 ENDSUBENT 36 0 A0480 199999 SUBENT A0480002 20200311 A094A0480 2 1 BIB 6 16 A0480 2 2 REACTION (92-U-233(A,N)94-PU-236,,SIG) A0480 2 3 DECAY-DATA (94-PU-236,2.7YR,A,,1.) A0480 2 4 SAMPLE The U-233 (isotopic purity of approximately 96 %, A0480 2 5 U-238 - 3%, U-234 <1%). Most of the targets were A0480 2 6 prepared by electrodeposition of 0.1 to 2 mg of A0480 2 7 hydrated uranium oxide over an area of about 1 cm**2 onA0480 2 8 a dish-shaped aluminum disk. The amount of deposited A0480 2 9 material was determined by direct alpha counting, A0480 2 10 weighting, or both. These targets were then mounted in A0480 2 11 a water-cooled micro-target holder which also served asA0480 2 12 a Faraday cup for beam intensity measurements. A0480 2 13 ERR-ANALYS (ERR-S) The deviation due to random error is believed A0480 2 14 to be about 10%. A0480 2 15 (ERR-T,15.,25.) Total errors A0480 2 16 STATUS (TABLE) Tbl. II from Phys.Rev.,111(1958)1358 A0480 2 17 HISTORY (20200311U) SD: STATUS updated. A0480 2 18 ENDBIB 16 0 A0480 2 19 COMMON 1 3 A0480 2 20 ERR-S A0480 2 21 PER-CENT A0480 2 22 10. A0480 2 23 ENDCOMMON 3 0 A0480 2 24 DATA 2 11 A0480 2 25 EN DATA A0480 2 26 MEV MB A0480 2 27 20.3 0.18 A0480 2 28 23.5 0.42 A0480 2 29 26.2 0.59 A0480 2 30 28.9 0.96 A0480 2 31 29.4 0.64 A0480 2 32 31.8 1.01 A0480 2 33 35.3 0.49 A0480 2 34 37.8 0.52 A0480 2 35 41.0 0.42 A0480 2 36 44.3 0.73 A0480 2 37 46.2 0.79 A0480 2 38 ENDDATA 13 0 A0480 2 39 ENDSUBENT 38 0 A0480 299999 SUBENT A0480003 20200311 A094A0480 3 1 BIB 6 16 A0480 3 2 REACTION (92-U-233(A,2N)94-PU-235,,SIG) A0480 3 3 DECAY-DATA (94-PU-235,26.MIN,A,,3.E-5) A0480 3 4 SAMPLE The U-233 (isotopic purity of approximately 96 %, A0480 3 5 U-238 - 3%, U-234 <1%). Most of the targets were A0480 3 6 prepared by electrodeposition of 0.1 to 2 mg of A0480 3 7 hydrated uranium oxide over an area of about 1 cm**2 onA0480 3 8 a dish-shaped aluminum disk. The amount of deposited A0480 3 9 material was determined by direct alpha counting, A0480 3 10 weighting, or both. These targets were then mounted in A0480 3 11 a water-cooled micro-target holder which also served asA0480 3 12 a Faraday cup for beam intensity measurements. A0480 3 13 ERR-ANALYS (ERR-S) The deviation due to random error is believed A0480 3 14 to be about 10%. A0480 3 15 (ERR-T,15.,25.) total error A0480 3 16 STATUS (TABLE) Tbl. II from Phys.Rev.,111(1958)1358 A0480 3 17 HISTORY (20200311U) SD: STATUS updated. A0480 3 18 ENDBIB 16 0 A0480 3 19 COMMON 1 3 A0480 3 20 ERR-S A0480 3 21 PER-CENT A0480 3 22 10. A0480 3 23 ENDCOMMON 3 0 A0480 3 24 DATA 2 8 A0480 3 25 EN DATA A0480 3 26 MEV MB A0480 3 27 23.5 1.30 A0480 3 28 26.2 3.68 A0480 3 29 28.9 6.54 A0480 3 30 31.8 3.40 A0480 3 31 35.3 1.19 A0480 3 32 37.8 0.94 A0480 3 33 41.0 1.19 A0480 3 34 46.2 1.31 A0480 3 35 ENDDATA 10 0 A0480 3 36 ENDSUBENT 35 0 A0480 399999 SUBENT A0480004 20200311 A094A0480 4 1 BIB 6 17 A0480 4 2 REACTION (92-U-233(A,3N)94-PU-234,,SIG) A0480 4 3 DECAY-DATA (94-PU-234,9.HR,A,,0.0616) A0480 4 4 SAMPLE The U-233 (isotopic purity of approximately 96 %, A0480 4 5 U-238 - 3%, U-234 <1%). Most of the targets were A0480 4 6 prepared by electrodeposition of 0.1 to 2 mg of A0480 4 7 hydrated uranium oxide over an area of about 1 cm**2 onA0480 4 8 a dish-shaped aluminum disk. The amount of deposited A0480 4 9 material was determined by direct alpha counting, A0480 4 10 weighting, or both. These targets were then mounted in A0480 4 11 a water-cooled micro-target holder which also served asA0480 4 12 a Faraday cup for beam intensity measurements. A0480 4 13 ERR-ANALYS (ERR-S) The deviation due to random error is believed A0480 4 14 to be about 10%. A0480 4 15 (ERR-T,15.,25.)Total errors A0480 4 16 STATUS (TABLE) Tbl. II from Phys.Rev.,111(1958)1358 A0480 4 17 HISTORY (20200311A) SD: Energy: 46.21, 46.22 -> 46.2 MeV as it A0480 4 18 is given in the Tbl.II. COMMENT deleted. STATUS updatedA0480 4 19 ENDBIB 17 0 A0480 4 20 COMMON 1 3 A0480 4 21 ERR-S A0480 4 22 PER-CENT A0480 4 23 10. A0480 4 24 ENDCOMMON 3 0 A0480 4 25 DATA 2 17 A0480 4 26 EN DATA A0480 4 27 MEV MB A0480 4 28 26.2 0.003 A0480 4 29 28.9 0.083 A0480 4 30 29.4 0.058 A0480 4 31 31.8 0.91 A0480 4 32 32.4 0.39 A0480 4 33 35.3 0.97 A0480 4 34 36.8 0.67 A0480 4 35 37.8 0.48 A0480 4 36 39.0 0.54 A0480 4 37 40.0 0.44 A0480 4 38 41.0 0.33 A0480 4 39 42.7 0.19 A0480 4 40 44.3 0.26 A0480 4 41 44.4 0.51 A0480 4 42 46.2 0.45 A0480 4 43 46.2 0.20 A0480 4 44 46.2 0.15 A0480 4 45 ENDDATA 19 0 A0480 4 46 ENDSUBENT 45 0 A0480 499999 SUBENT A0480005 20200311 A094A0480 5 1 BIB 6 16 A0480 5 2 REACTION (92-U-233(A,4N)94-PU-233,,SIG) A0480 5 3 DECAY-DATA (94-PU-233,20.MIN,A,,0.0012) A0480 5 4 SAMPLE The U-233 (isotopic purity of approximately 96 %, A0480 5 5 U-238 - 3%, U-234 <1%). Most of the targets were A0480 5 6 prepared by electrodeposition of 0.1 to 2 mg of A0480 5 7 hydrated uranium oxide over an area of about 1 cm**2 onA0480 5 8 a dish-shaped aluminum disk. The amount of deposited A0480 5 9 material was determined by direct alpha counting, A0480 5 10 weighting, or both. These targets were then mounted in A0480 5 11 a water-cooled micro-target holder which also served asA0480 5 12 a Faraday cup for beam intensity measurements. A0480 5 13 ERR-ANALYS (DATA-ERR,,50.) This product was difficult to measure A0480 5 14 and the limits of error may be as much as 50%. A0480 5 15 STATUS (TABLE) Tbl. II from Phys.Rev.,111(1958)1358 A0480 5 16 HISTORY (20200311A) SD: Energy: 46.21, 46.22 -> 46.2 MeV as it A0480 5 17 is given in the Tbl.II. COMMENT deleted. STATUS updatedA0480 5 18 ENDBIB 16 0 A0480 5 19 NOCOMMON 0 0 A0480 5 20 DATA 2 5 A0480 5 21 EN DATA A0480 5 22 MEV MB A0480 5 23 42.7 0.27 A0480 5 24 44.4 1.03 A0480 5 25 46.2 1.13 A0480 5 26 46.2 0.33 A0480 5 27 46.2 0.34 A0480 5 28 ENDDATA 7 0 A0480 5 29 ENDSUBENT 28 0 A0480 599999 SUBENT A0480006 20200311 A094A0480 6 1 BIB 6 16 A0480 6 2 REACTION (92-U-233(A,5N)94-PU-232,,SIG) A0480 6 3 DECAY-DATA (94-PU-232,30.MIN,A,,0.11) A0480 6 4 SAMPLE The U-233 (isotopic purity of approximately 96 %, A0480 6 5 U-238 - 3%, U-234 <1%). Most of the targets were A0480 6 6 prepared by electrodeposition of 0.1 to 2 mg of A0480 6 7 hydrated uranium oxide over an area of about 1 cm**2 onA0480 6 8 a dish-shaped aluminum disk. The amount of deposited A0480 6 9 material was determined by direct alpha counting, A0480 6 10 weighting, or both. These targets were then mounted in A0480 6 11 a water-cooled micro-target holder which also served asA0480 6 12 a Faraday cup for beam intensity measurements. A0480 6 13 ERR-ANALYS (ERR-S) The deviation due to random error is believed A0480 6 14 to be about 10%. A0480 6 15 (ERR-T,15.,25.)Total errors A0480 6 16 STATUS (TABLE) Tbl. II from Phys.Rev.,111(1958)1358 A0480 6 17 HISTORY (20200311U) SD: STATUS updated. A0480 6 18 ENDBIB 16 0 A0480 6 19 COMMON 1 3 A0480 6 20 ERR-S A0480 6 21 PER-CENT A0480 6 22 10. A0480 6 23 ENDCOMMON 3 0 A0480 6 24 DATA 2 1 A0480 6 25 EN DATA A0480 6 26 MEV MB A0480 6 27 42.7 0.002 A0480 6 28 ENDDATA 3 0 A0480 6 29 ENDSUBENT 28 0 A0480 699999 SUBENT A0480007 20200311 A094A0480 7 1 BIB 7 19 A0480 7 2 REACTION (92-U-233(A,P)93-NP-236-M,,SIG) A0480 7 3 DECAY-DATA 9236-M,22.HR,B-,,1.) A0480 7 4 SAMPLE The U-233 (isotopic purity of approximately 96 %, A0480 7 5 U-238 - 3%, U-234 <1%). Most of the targets were A0480 7 6 prepared by electrodeposition of 0.1 to 2 mg of A0480 7 7 hydrated uranium oxide over an area of about 1 cm**2 onA0480 7 8 a dish-shaped aluminum disk. The amount of deposited A0480 7 9 material was determined by direct alpha counting, A0480 7 10 weighting, or both. These targets were then mounted in A0480 7 11 a water-cooled micro-target holder which also served asA0480 7 12 a Faraday cup for beam intensity measurements. A0480 7 13 ERR-ANALYS (ERR-S) The deviation due to random error is believed A0480 7 14 to be about 10%. A0480 7 15 (ERR-T,15.,25.)Total errors A0480 7 16 STATUS (TABLE) Tbl. II from Phys.Rev.,111(1958)1358 A0480 7 17 COMMENT /By authors/ detector efficiency =92+-20% A0480 7 18 HISTORY (20160317A) SD: SF4=Np-236m1 -> Np-236m in REACTION A0480 7 19 code and DECAY-DATA. A0480 7 20 (20200311U) SD: STATUS updated. A0480 7 21 ENDBIB 19 0 A0480 7 22 COMMON 1 3 A0480 7 23 ERR-S A0480 7 24 PER-CENT A0480 7 25 10. A0480 7 26 ENDCOMMON 3 0 A0480 7 27 DATA 2 16 A0480 7 28 EN DATA A0480 7 29 MEV MB A0480 7 30 26.2 0.20 A0480 7 31 28.9 0.53 A0480 7 32 30.7 0.63 A0480 7 33 31.8 1.72 A0480 7 34 32.4 0.64 A0480 7 35 34.3 1.07 A0480 7 36 35.3 0.58 A0480 7 37 36.8 1.46 A0480 7 38 37.8 0.74 A0480 7 39 40.4 0.40 A0480 7 40 41.0 0.62 A0480 7 41 42.7 0.70 A0480 7 42 43.8 2.53 A0480 7 43 44.3 0.74 A0480 7 44 44.4 0.72 A0480 7 45 46.2 0.30 A0480 7 46 ENDDATA 18 0 A0480 7 47 ENDSUBENT 46 0 A0480 799999 SUBENT A0480008 20200311 A094A0480 8 1 BIB 7 17 A0480 8 2 REACTION (92-U-233(A,X)93-NP-235,,SIG) A0480 8 3 SAMPLE The U-233 (isotopic purity of approximately 96%, A0480 8 4 U-238 - 3%, U-234 <1%). Most of the targets were A0480 8 5 prepared by electrodeposition of 0.1 to 2 mg of A0480 8 6 hydrated uranium oxide over an area of about 1 cm**2 onA0480 8 7 a dish-shaped aluminum disk. The amount of deposited A0480 8 8 material was determined by direct alpha counting, A0480 8 9 weighting, or both. These targets were then mounted in A0480 8 10 a water-cooled micro-target holder which also served asA0480 8 11 a Faraday cup for beam intensity measurements. A0480 8 12 ERR-ANALYS (DATA-ERR,,50.) This product was difficult to measure A0480 8 13 and the limits of error may be as much as 50%. A0480 8 14 DECAY-DATA (93-NP-235,410.D,EC,,1.) A0480 8 15 COMMENT /By authors/. detector efficiency =41+-4 %. A0480 8 16 STATUS (TABLE) Tbl. II from Phys.Rev.,111(1958)1358 A0480 8 17 HISTORY (20160317A) SD: SF3=N+P -> X in REACTION code. A0480 8 18 (20200311U) SD: STATUS updated. A0480 8 19 ENDBIB 17 0 A0480 8 20 NOCOMMON 0 0 A0480 8 21 DATA 2 14 A0480 8 22 EN DATA A0480 8 23 MEV MB A0480 8 24 26.2 1.0 A0480 8 25 28.9 -1.8 A0480 8 26 30.7 3.5 A0480 8 27 31.8 0.3 A0480 8 28 34.3 13.5 A0480 8 29 35.3 2.5 A0480 8 30 36.8 6.5 A0480 8 31 37.8 3.5 A0480 8 32 40.4 4.6 A0480 8 33 41.0 14.9 A0480 8 34 42.7 2.6 A0480 8 35 43.8 8.8 A0480 8 36 44.3 18.7 A0480 8 37 46.2 21.3 A0480 8 38 ENDDATA 16 0 A0480 8 39 ENDSUBENT 38 0 A0480 899999 SUBENT A0480009 20200311 A094A0480 9 1 BIB 7 18 A0480 9 2 REACTION (92-U-233(A,X)93-NP-234,,SIG) A0480 9 3 DECAY-DATA (93-NP-234,4.4D,EC,,1.) A0480 9 4 SAMPLE The U-233 (isotopic purity of approximately 96 %, A0480 9 5 U-238 - 3%, U-234 <1%). Most of the targets were A0480 9 6 prepared by electrodeposition of 0.1 to 2 mg of A0480 9 7 hydrated uranium oxide over an area of about 1 cm**2 onA0480 9 8 a dish-shaped aluminum disk. The amount of deposited A0480 9 9 material was determined by direct alpha counting, A0480 9 10 weighting, or both. These targets were then mounted in A0480 9 11 a water-cooled micro-target holder which also served asA0480 9 12 a Faraday cup for beam intensity measurements. A0480 9 13 ERR-ANALYS (ERR-S) The deviation due to random error is believed A0480 9 14 to be about 10%. A0480 9 15 (ERR-T,15.,25.)Total errors A0480 9 16 COMMENT /By authors/ detector efficiency =92+-20% A0480 9 17 STATUS (TABLE) Tbl. II from Phys.Rev.,111(1958)1358 A0480 9 18 HISTORY (20160317A) SD: SF3=2N+P -> X in REACTION code. A0480 9 19 (20200311U) SD: STATUS updated. A0480 9 20 ENDBIB 18 0 A0480 9 21 COMMON 1 3 A0480 9 22 ERR-S A0480 9 23 PER-CENT A0480 9 24 10. A0480 9 25 ENDCOMMON 3 0 A0480 9 26 DATA 2 16 A0480 9 27 EN DATA A0480 9 28 MEV MB A0480 9 29 26.2 0.16 A0480 9 30 28.9 1.63 A0480 9 31 30.7 5.04 A0480 9 32 31.8 4.91 A0480 9 33 32.4 3.52 A0480 9 34 34.3 10.9 A0480 9 35 35.3 5.20 A0480 9 36 36.8 10.5 A0480 9 37 37.8 7.25 A0480 9 38 40.4 10.4 A0480 9 39 41.0 11.8 A0480 9 40 42.7 9.4 A0480 9 41 43.8 17.8 A0480 9 42 44.3 19.9 A0480 9 43 44.4 15.9 A0480 9 44 46.2 19.6 A0480 9 45 ENDDATA 18 0 A0480 9 46 ENDSUBENT 45 0 A0480 999999 SUBENT A0480010 20200311 A094A0480 10 1 BIB 7 18 A0480 10 2 REACTION (92-U-233(A,X)93-NP-233,,SIG) A0480 10 3 DECAY-DATA (93-NP-233,35.MIN,EC,,1.) A0480 10 4 SAMPLE The U-233 (isotopic purity of approximately 96 %, A0480 10 5 U-238 - 3%, U-234 <1%). Most of the targets were A0480 10 6 prepared by electrodeposition of 0.1 to 2 mg of A0480 10 7 hydrated uranium oxide over an area of about 1 cm**2 onA0480 10 8 a dish-shaped aluminum disk. The amount of deposited A0480 10 9 material was determined by direct alpha counting, A0480 10 10 weighting, or both. These targets were then mounted in A0480 10 11 a water-cooled micro-target holder which also served asA0480 10 12 a Faraday cup for beam intensity measurements. A0480 10 13 ERR-ANALYS (ERR-S) The deviation due to random error is believed A0480 10 14 to be about 10%. A0480 10 15 (ERR-T,15.,25.) Total errors A0480 10 16 COMMENT /By authors/ detector efficiency =20+-20% A0480 10 17 STATUS (TABLE) Tbl. II from Phys.Rev.,111(1958)1358 A0480 10 18 HISTORY (20160317A) SD: SF3=3N+P -> X in REACTION code. A0480 10 19 (20200311U) SD: STATUS updated. A0480 10 20 ENDBIB 18 0 A0480 10 21 COMMON 1 3 A0480 10 22 ERR-S A0480 10 23 PER-CENT A0480 10 24 10. A0480 10 25 ENDCOMMON 3 0 A0480 10 26 DATA 2 8 A0480 10 27 EN DATA A0480 10 28 MEV MB A0480 10 29 35.3 0.21 A0480 10 30 37.8 0.11 A0480 10 31 40.4 1.16 A0480 10 32 41.0 0.60 A0480 10 33 43.8 1.41 A0480 10 34 44.3 1.72 A0480 10 35 44.4 0.64 A0480 10 36 46.2 1.10 A0480 10 37 ENDDATA 10 0 A0480 10 38 ENDSUBENT 37 0 A0480 1099999 SUBENT A0480011 20200311 A094A0480 11 1 BIB 7 17 A0480 11 2 REACTION (92-U-235(A,N)94-PU-238,,SIG) A0480 11 3 COMMENT Spallation cross sections A0480 11 4 DECAY-DATA (94-PU-238,89.6YR,A,,1.) A0480 11 5 SAMPLE The U-235 with isotopic purity > 99.9% used. Most of A0480 11 6 the targets were prepared by electrodeposition of 0.1 A0480 11 7 to 2 mg of hydrated uranium oxide over an area of aboutA0480 11 8 1 cm**2 on a dish-shaped aluminum disk. The amount of A0480 11 9 deposited material was determined by direct alpha A0480 11 10 counting, weighting, or both. These targets were then A0480 11 11 mounted in a water-cooled microtarget holder which alsoA0480 11 12 served as a Faraday cup for beam intensity measurementsA0480 11 13 ERR-ANALYS (ERR-S) The deviation due to random error is believed A0480 11 14 to be about 10%. A0480 11 15 (ERR-T) total error A0480 11 16 STATUS (TABLE) Tbl. III from Phys.Rev.,111(1958)1358; A0480 11 17 same data in Tbl.III of UCRL-3858,1957 A0480 11 18 HISTORY (20200311U) SD: STATUS, ERR-ANALYS updated. A0480 11 19 ENDBIB 17 0 A0480 11 20 COMMON 2 3 A0480 11 21 ERR-S ERR-T A0480 11 22 PER-CENT PER-CENT A0480 11 23 10. 25. A0480 11 24 ENDCOMMON 3 0 A0480 11 25 DATA 2 9 A0480 11 26 EN DATA A0480 11 27 MEV MB A0480 11 28 18.7 0.27 A0480 11 29 21.9 0.36 A0480 11 30 23.6 1.32 A0480 11 31 27.3 1.74 A0480 11 32 30.6 1.42 A0480 11 33 34.1 2.15 A0480 11 34 39.5 2.26 A0480 11 35 42.8 2.52 A0480 11 36 45.4 0.91 A0480 11 37 ENDDATA 11 0 A0480 11 38 ENDSUBENT 37 0 A0480 1199999 SUBENT A0480012 20200311 A094A0480 12 1 BIB 6 16 A0480 12 2 REACTION (92-U-235(A,2N)94-PU-237,,SIG) A0480 12 3 DECAY-DATA (94-PU-237-G,44.D,A,,3.3E-5) A0480 12 4 SAMPLE The U-235 with isotopic purity > 99.9% used. Most of A0480 12 5 the targets were prepared by electrodeposition of 0.1 A0480 12 6 to 2 mg of hydrated uranium oxide over an area of aboutA0480 12 7 1 cm**2 on a dish-shaped aluminum disk. The amount of A0480 12 8 deposited material was determined by direct alpha A0480 12 9 counting, weighting, or both. These targets were then A0480 12 10 mounted in a water-cooled microtarget holder which alsoA0480 12 11 served as a Faraday cup for beam intensity measurementsA0480 12 12 ERR-ANALYS (ERR-S) The deviation due to random error is believed A0480 12 13 to be about 10%. A0480 12 14 (ERR-T) total error A0480 12 15 STATUS (TABLE) Tbl. III from Phys.Rev.,111(1958)1358; A0480 12 16 same data in Tbl.III of UCRL-3858,1957 A0480 12 17 HISTORY (20200311U) SD: STATUS, ERR-ANALYS updated. A0480 12 18 ENDBIB 16 0 A0480 12 19 COMMON 2 3 A0480 12 20 ERR-S ERR-T A0480 12 21 PER-CENT PER-CENT A0480 12 22 10. 15. A0480 12 23 ENDCOMMON 3 0 A0480 12 24 DATA 2 9 A0480 12 25 EN DATA A0480 12 26 MEV MB A0480 12 27 21.9 4.43 A0480 12 28 23.6 13.3 A0480 12 29 27.3 15.8 A0480 12 30 30.0 8.3 A0480 12 31 30.6 6.84 A0480 12 32 34.7 6.8 A0480 12 33 39.5 5.65 A0480 12 34 42.8 4.8 A0480 12 35 45.4 3.5 A0480 12 36 ENDDATA 11 0 A0480 12 37 ENDSUBENT 36 0 A0480 1299999 SUBENT A0480013 20200311 A094A0480 13 1 BIB 6 16 A0480 13 2 REACTION (92-U-235(A,3N)94-PU-236,,SIG) A0480 13 3 DECAY-DATA (94-PU-236,2.7YR,A,,1.) A0480 13 4 SAMPLE The U-235 with isotopic purity > 99.9% used. Most of A0480 13 5 the targets were prepared by electrodeposition of 0.1 A0480 13 6 to 2 mg of hydrated uranium oxide over an area of aboutA0480 13 7 1 cm**2 on a dish-shaped aluminum disk. The amount of A0480 13 8 deposited material was determined by direct alpha A0480 13 9 counting, weighting, or both. These targets were then A0480 13 10 mounted in a water-cooled microtarget holder which alsoA0480 13 11 served as a Faraday cup for beam intensity measurementsA0480 13 12 ERR-ANALYS (ERR-S) The deviation due to random error is believed A0480 13 13 to be about 10%. A0480 13 14 (ERR-T) total error A0480 13 15 STATUS (TABLE) Tbl. III from Phys.Rev.,111(1958)1358; A0480 13 16 same data in Tbl.III of UCRL-3858,1957 A0480 13 17 HISTORY (20200311U) SD: STATUS, ERR-ANALYS updated. A0480 13 18 ENDBIB 16 0 A0480 13 19 COMMON 2 3 A0480 13 20 ERR-S ERR-T A0480 13 21 PER-CENT PER-CENT A0480 13 22 10. 15. A0480 13 23 ENDCOMMON 3 0 A0480 13 24 DATA 2 9 A0480 13 25 EN DATA A0480 13 26 MEV MB A0480 13 27 27.3 0.61 A0480 13 28 30.0 4.43 A0480 13 29 30.6 4.15 A0480 13 30 34.1 8.63 A0480 13 31 34.7 7.23 A0480 13 32 37.1 3.67 A0480 13 33 39.5 3.12 A0480 13 34 42.8 2.23 A0480 13 35 45.4 1.86 A0480 13 36 ENDDATA 11 0 A0480 13 37 ENDSUBENT 36 0 A0480 1399999 SUBENT A0480014 20200311 A094A0480 14 1 BIB 7 17 A0480 14 2 REACTION (92-U-235(A,4N)94-PU-235,,SIG) A0480 14 3 DECAY-DATA (94-PU-235,26.MIN,A,,3.E-5) A0480 14 4 SAMPLE The U-235 with isotopic purity > 99.9% used. Most of A0480 14 5 the targets were prepared by electrodeposition of 0.1 A0480 14 6 to 2 mg of hydrated uranium oxide over an area of aboutA0480 14 7 1 cm**2 on a dish-shaped aluminum disk. The amount of A0480 14 8 deposited material was determined by direct alpha A0480 14 9 counting, weighting, or both. These targets were then A0480 14 10 mounted in a water-cooled microtarget holder which alsoA0480 14 11 served as a Faraday cup for beam intensity measurementsA0480 14 12 COMMENT /By authors/ detector efficiency =70+-14% A0480 14 13 ERR-ANALYS (ERR-S) The deviation due to random error is believed A0480 14 14 to be about 10%. A0480 14 15 (ERR-T) total error A0480 14 16 STATUS (TABLE) Tbl. III from Phys.Rev.,111(1958)1358; A0480 14 17 same data in Tbl.III of UCRL-3858,1957 A0480 14 18 HISTORY (20200311U) SD: STATUS, ERR-ANALYS updated. A0480 14 19 ENDBIB 17 0 A0480 14 20 COMMON 2 3 A0480 14 21 ERR-S ERR-T A0480 14 22 PER-CENT PER-CENT A0480 14 23 10. 15. A0480 14 24 ENDCOMMON 3 0 A0480 14 25 DATA 2 4 A0480 14 26 EN DATA A0480 14 27 MEV MB A0480 14 28 37.1 0.17 A0480 14 29 39.5 1.5 A0480 14 30 42.8 2.4 A0480 14 31 45.4 1.55 A0480 14 32 ENDDATA 6 0 A0480 14 33 ENDSUBENT 32 0 A0480 1499999 SUBENT A0480015 20200311 A094A0480 15 1 BIB 6 16 A0480 15 2 REACTION (92-U-235(A,5N)94-PU-234,,SIG) A0480 15 3 DECAY-DATA (94-PU-234,9.HR,A,,0.0616) A0480 15 4 SAMPLE The U-235 with isotopic purity > 99.9% used. Most of A0480 15 5 the targets were prepared by electrodeposition of 0.1 A0480 15 6 to 2 mg of hydrated uranium oxide over an area of aboutA0480 15 7 1 cm**2 on a dish-shaped aluminum disk. The amount of A0480 15 8 deposited material was determined by direct alpha A0480 15 9 counting, weighting, or both. These targets were then A0480 15 10 mounted in a water-cooled microtarget holder which alsoA0480 15 11 served as a Faraday cup for beam intensity measurementsA0480 15 12 ERR-ANALYS (ERR-S) The deviation due to random error is believed A0480 15 13 to be about 10%. A0480 15 14 (ERR-T) total error A0480 15 15 STATUS (TABLE) Tbl. III from Phys.Rev.,111(1958)1358; A0480 15 16 same data in Tbl.III of UCRL-3858,1957 A0480 15 17 HISTORY (20200311U) SD: STATUS, ERR-ANALYS updated. A0480 15 18 ENDBIB 16 0 A0480 15 19 COMMON 2 3 A0480 15 20 ERR-S ERR-T A0480 15 21 PER-CENT PER-CENT A0480 15 22 10. 15. A0480 15 23 ENDCOMMON 3 0 A0480 15 24 DATA 2 2 A0480 15 25 EN DATA A0480 15 26 MEV MB A0480 15 27 42.8 0.002 A0480 15 28 45.4 0.034 A0480 15 29 ENDDATA 4 0 A0480 15 30 ENDSUBENT 29 0 A0480 1599999 SUBENT A0480016 20200311 A094A0480 16 1 BIB 7 18 A0480 16 2 REACTION (92-U-235(A,P)93-NP-238,,SIG) A0480 16 3 DECAY-DATA (93-NP-238,2.1D,B-,,1.) A0480 16 4 SAMPLE The U-235 with isotopic purity > 99.9% used. Most of A0480 16 5 the targets were prepared by electrodeposition of 0.1 A0480 16 6 to 2 mg of hydrated uranium oxide over an area of aboutA0480 16 7 1 cm**2 on a dish-shaped aluminum disk. The amount of A0480 16 8 deposited material was determined by direct alpha A0480 16 9 counting, weighting, or both. These targets were then A0480 16 10 mounted in a water-cooled microtarget holder which alsoA0480 16 11 served as a Faraday cup for beam intensity measurementsA0480 16 12 ERR-ANALYS (ERR-S) The deviation due to random error is believed A0480 16 13 to be about 10%. A0480 16 14 (ERR-T) total error A0480 16 15 COMMENT /By authors/. detector efficiency =70+- 5%. A0480 16 16 STATUS (TABLE) Tbl. III from Phys.Rev.,111(1958)1358; A0480 16 17 same data in Tbl.III of UCRL-3858,1957 A0480 16 18 HISTORY (20160317A) SD: SF5=IND deleted from REACTION code. A0480 16 19 (20200311U) SD: STATUS, ERR-ANALYS updated. A0480 16 20 ENDBIB 18 0 A0480 16 21 COMMON 2 3 A0480 16 22 ERR-S ERR-T A0480 16 23 PER-CENT PER-CENT A0480 16 24 10. 15. A0480 16 25 ENDCOMMON 3 0 A0480 16 26 DATA 2 12 A0480 16 27 EN DATA A0480 16 28 MEV MB A0480 16 29 21.9 0.02 A0480 16 30 23.6 0.035 A0480 16 31 25.2 1.01 A0480 16 32 27.3 0.55 A0480 16 33 29.7 1.7 A0480 16 34 30.0 1.43 A0480 16 35 30.6 1.57 A0480 16 36 34.1 2.08 A0480 16 37 37.1 1.92 A0480 16 38 39.5 1.87 A0480 16 39 42.8 1.94 A0480 16 40 45.4 1.21 A0480 16 41 ENDDATA 14 0 A0480 16 42 ENDSUBENT 41 0 A0480 1699999 SUBENT A0480017 20200311 A094A0480 17 1 BIB 7 20 A0480 17 2 REACTION (92-U-235(A,X)93-NP-236-M,,SIG) A0480 17 3 DECAY-DATA (93-NP-236-M,22.HR,B-,,1.) A0480 17 4 SAMPLE The U-235 with isotopic purity > 99.9% used. Most of A0480 17 5 the targets were prepared by electrodeposition of 0.1 A0480 17 6 to 2 mg of hydrated uranium oxide over an area of aboutA0480 17 7 1 cm**2 on a dish-shaped aluminum disk. The amount of A0480 17 8 deposited material was determined by direct alpha A0480 17 9 counting, weighting, or both. These targets were then A0480 17 10 mounted in a water-cooled microtarget holder which alsoA0480 17 11 served as a Faraday cup for beam intensity measurementsA0480 17 12 ERR-ANALYS (ERR-S) The deviation due to random error is believed A0480 17 13 to be about 10%. A0480 17 14 (ERR-T) total error A0480 17 15 COMMENT /By authors/ detector efficiency =92+-20%. A0480 17 16 STATUS (TABLE) Tbl. III from Phys.Rev.,111(1958)1358; A0480 17 17 same data in Tbl.III of UCRL-3858,1957 A0480 17 18 HISTORY (20160317A) SD: SF3=2N+P -> X, SF4=Np-236m1 -> Np-236m A0480 17 19 in REACTION code and DECAY-DATA. A0480 17 20 (20160317A) SD: SF5=IND deleted from REACTION code. A0480 17 21 (20200311U) SD: STATUS, ERR-ANALYS updated. A0480 17 22 ENDBIB 20 0 A0480 17 23 COMMON 2 3 A0480 17 24 ERR-S ERR-T A0480 17 25 PER-CENT PER-CENT A0480 17 26 10. 15. A0480 17 27 ENDCOMMON 3 0 A0480 17 28 DATA 2 12 A0480 17 29 EN DATA A0480 17 30 MEV MB A0480 17 31 23.6 0.042 A0480 17 32 25.2 0.087 A0480 17 33 27.3 0.52 A0480 17 34 29.7 1.86 A0480 17 35 30.0 2.22 A0480 17 36 30.6 2.38 A0480 17 37 34.1 4.38 A0480 17 38 34.7 4.20 A0480 17 39 37.1 5.9 A0480 17 40 39.5 8.5 A0480 17 41 42.8 10.7 A0480 17 42 45.4 10.5 A0480 17 43 ENDDATA 14 0 A0480 17 44 ENDSUBENT 43 0 A0480 1799999 SUBENT A0480018 20200311 A094A0480 18 1 BIB 8 21 A0480 18 2 REACTION (92-U-238(A,X)93-NP-240-M,,SIG) A0480 18 3 DECAY-DATA (93-NP-240-G,60.MIN,B-,,1.) (now known as the ground A0480 18 4 state) A0480 18 5 SAMPLE U-238 with isotopic purity > 99.% used. Most of A0480 18 6 the targets were prepared by electrodeposition of 0.1 A0480 18 7 to 2 mg of hydrated uranium oxide over an area of aboutA0480 18 8 1 cm**2 on a dish-shaped aluminum disk. The amount of A0480 18 9 deposited material was determined by direct alpha A0480 18 10 counting, weighting, or both. These targets were then A0480 18 11 mounted in a water-cooled microtarget holder which alsoA0480 18 12 served as a Faraday cup for beam intensity measurementsA0480 18 13 CORRECTION Appropriate correction factors were applied to obtain A0480 18 14 disintegration rates from the measured counting rates. A0480 18 15 ERR-ANALYS (ERR-S) The deviation due to random error is believed A0480 18 16 to be about 10%. A0480 18 17 (ERR-T,15.,25.)Total errors A0480 18 18 COMMENT /By authors/ detector efficiency =94+- 6%. A0480 18 19 STATUS (TABLE) Tbl. IV from Phys.Rev.,111(1958)1358 A0480 18 20 HISTORY (20160317A) SD: SF3=N+P -> X, SF4=Np-240m1 -> Np-240m A0480 18 21 in REACTION code and DECAY-DATA. A0480 18 22 (20200311U) SD: STATUS updated. A0480 18 23 ENDBIB 21 0 A0480 18 24 COMMON 1 3 A0480 18 25 ERR-S A0480 18 26 PER-CENT A0480 18 27 10. A0480 18 28 ENDCOMMON 3 0 A0480 18 29 DATA 2 9 A0480 18 30 EN DATA A0480 18 31 MEV MB A0480 18 32 22.6 0.024 A0480 18 33 25.2 1.1 A0480 18 34 27.1 1.2 A0480 18 35 32.5 1.7 A0480 18 36 33.8 3.6 A0480 18 37 37.9 6.0 A0480 18 38 38.6 6.1 A0480 18 39 41.4 6.3 A0480 18 40 45.4 5.3 A0480 18 41 ENDDATA 11 0 A0480 18 42 ENDSUBENT 41 0 A0480 1899999 SUBENT A0480019 20200311 A094A0480 19 1 BIB 8 19 A0480 19 2 REACTION (92-U-238(A,X)93-NP-239,,SIG) A0480 19 3 DECAY-DATA (93-NP-239,2.3D,B-,,1.) A0480 19 4 SAMPLE U-238 with isotopic purity > 99.% used. Most of A0480 19 5 the targets were prepared by electrodeposition of 0.1 A0480 19 6 to 2 mg of hydrated uranium oxide over an area of aboutA0480 19 7 1 cm**2 on a dish-shaped aluminum disk. The amount of A0480 19 8 deposited material was determined by direct alpha A0480 19 9 counting, weighting, or both. These targets were then A0480 19 10 mounted in a water-cooled microtarget holder which alsoA0480 19 11 served as a Faraday cup for beam intensity measurementsA0480 19 12 ERR-ANALYS (ERR-S) The deviation due to random error is believed A0480 19 13 to be about 10%. A0480 19 14 (ERR-T,15.,25.)Total errors A0480 19 15 FLAG (1.)The results of two measurements had been include A0480 19 16 for data table by authors. A0480 19 17 COMMENT /By authors/. detector efficiency =92+- 5%. A0480 19 18 STATUS (TABLE) Tbl. IV from Phys.Rev.,111(1958)1358 A0480 19 19 HISTORY (20160317A) SD: SF3=2N+P -> X in REACTION code. A0480 19 20 (20200311U) SD: STATUS updated. A0480 19 21 ENDBIB 19 0 A0480 19 22 COMMON 1 3 A0480 19 23 ERR-S A0480 19 24 PER-CENT A0480 19 25 10. A0480 19 26 ENDCOMMON 3 0 A0480 19 27 DATA 3 9 A0480 19 28 EN DATA FLAG A0480 19 29 MEV MB NO-DIM A0480 19 30 22.6 0.22 A0480 19 31 25.2 1.06 A0480 19 32 27.1 9.1 A0480 19 33 32.5 9.0 A0480 19 34 33.8 9.3 A0480 19 35 38.6 17.5 1. A0480 19 36 38.6 20.5 1. A0480 19 37 41.4 21.2 A0480 19 38 45.4 33.4 A0480 19 39 ENDDATA 11 0 A0480 19 40 ENDSUBENT 39 0 A0480 1999999 SUBENT A0480020 20200311 A094A0480 20 1 BIB 7 17 A0480 20 2 REACTION (92-U-238(A,X)93-NP-238,,SIG) A0480 20 3 DECAY-DATA (93-NP-238,2.1D,B-,,1.) A0480 20 4 SAMPLE U-238 with isotopic purity > 99.% used. Most of A0480 20 5 the targets were prepared by electrodeposition of 0.1 A0480 20 6 to 2 mg of hydrated uranium oxide over an area of aboutA0480 20 7 1 cm**2 on a dish-shaped aluminum disk. The amount of A0480 20 8 deposited material was determined by direct alpha A0480 20 9 counting, weighting, or both. These targets were then A0480 20 10 mounted in a water-cooled microtarget holder which alsoA0480 20 11 served as a Faraday cup for beam intensity measurementsA0480 20 12 ERR-ANALYS (ERR-S) The deviation due to random error is believed A0480 20 13 to be about 10%. A0480 20 14 (ERR-T,15.,25.)Total errors A0480 20 15 COMMENT /By authors/ detector efficiency =70+- 5%. A0480 20 16 STATUS (TABLE) Tbl. IV from Phys.Rev.,111(1958)1358 A0480 20 17 HISTORY (20160317A) SD: SF3=3N+P -> X in REACTION code. A0480 20 18 (20200311U) SD: STATUS updated. A0480 20 19 ENDBIB 17 0 A0480 20 20 COMMON 1 3 A0480 20 21 ERR-S A0480 20 22 PER-CENT A0480 20 23 10. A0480 20 24 ENDCOMMON 3 0 A0480 20 25 DATA 2 2 A0480 20 26 EN DATA A0480 20 27 MEV MB A0480 20 28 40.0 3.8 A0480 20 29 45.4 8.8 A0480 20 30 ENDDATA 4 0 A0480 20 31 ENDSUBENT 30 0 A0480 2099999 SUBENT A0480021 20200311 A094A0480 21 1 BIB 7 17 A0480 21 2 REACTION (92-U-238(A,X)92-U-237,,SIG) A0480 21 3 DECAY-DATA (92-U-237,6.75D,B-,,1.) A0480 21 4 SAMPLE U-238 with isotopic purity > 99.% used. Most of A0480 21 5 the targets were prepared by electrodeposition of 0.1 A0480 21 6 to 2 mg of hydrated uranium oxide over an area of aboutA0480 21 7 1 cm**2 on a dish-shaped aluminum disk. The amount of A0480 21 8 deposited material was determined by direct alpha A0480 21 9 counting, weighting, or both. These targets were then A0480 21 10 mounted in a water-cooled microtarget holder which alsoA0480 21 11 served as a Faraday cup for beam intensity measurementsA0480 21 12 ERR-ANALYS (ERR-S) The deviation due to random error is believed A0480 21 13 to be about 10%. A0480 21 14 (ERR-T,15.,25.)Total errors A0480 21 15 COMMENT /By authors/ detector efficiency =80+- 5%. A0480 21 16 STATUS (TABLE) Tbl. IV from Phys.Rev.,111(1958)1358 A0480 21 17 HISTORY (20160317A) SD: SF3=N+A -> X in REACTION code. A0480 21 18 (20200311U) SD: STATUS updated. FLAG deleted. A0480 21 19 ENDBIB 17 0 A0480 21 20 COMMON 1 3 A0480 21 21 ERR-S A0480 21 22 PER-CENT A0480 21 23 10. A0480 21 24 ENDCOMMON 3 0 A0480 21 25 DATA 2 8 A0480 21 26 EN DATA A0480 21 27 MEV MB A0480 21 28 25.2 0.6 A0480 21 29 27.1 1.5 A0480 21 30 32.5 8.2 A0480 21 31 33.8 7.9 A0480 21 32 38.6 49.2 A0480 21 33 38.6 56.2 A0480 21 34 43.9 56.0 A0480 21 35 45.4 74. A0480 21 36 ENDDATA 10 0 A0480 21 37 ENDSUBENT 36 0 A0480 2199999 SUBENT A0480022 20200311 A094A0480 22 1 BIB 6 21 A0480 22 2 REACTION (92-U-233(A,F)MASS,CHN,SIG) A0480 22 3 SAMPLE The U-233 (isotopic purity of approximately 96%, A0480 22 4 U-238 - 3%, U-234 <1%). Most of the targets were A0480 22 5 prepared by electrodeposition of 0.1 to 2 mg of A0480 22 6 hydrated uranium oxide over an area of about 1 cm**2 onA0480 22 7 a dish-shaped aluminum disk. The amount of deposited A0480 22 8 material was determined by direct alpha counting, A0480 22 9 weighting, or both. These targets were then mounted in A0480 22 10 a water-cooled micro-target holder which also served asA0480 22 11 a Faraday cup for beam intensity measurements. A0480 22 12 ANALYSIS (CHGDS) A0480 22 13 ERR-ANALYS (DATA-ERR) The limits of error are estimated to be A0480 22 14 about 15% for most of the mass chains reported. A0480 22 15 However, at higher energies, the chain yield A0480 22 16 corrections become quite sizeable and the errors A0480 22 17 may be somewhat greater. A0480 22 18 STATUS (TABLE) Tbl. V from Phys.Rev.,111(1958)1358 A0480 22 19 HISTORY (20160317A) SD: SF5=CUM -> CHN in REACTION code. A0480 22 20 ANALYSIS added. A0480 22 21 (20200311A) SD: Data from Subents 023-030 were added. A0480 22 22 STATUS updated. A0480 22 23 ENDBIB 21 0 A0480 22 24 COMMON 1 3 A0480 22 25 DATA-ERR A0480 22 26 PER-CENT A0480 22 27 15. A0480 22 28 ENDCOMMON 3 0 A0480 22 29 DATA 4 86 A0480 22 30 EN MASS DATA DATA-MIN A0480 22 31 MEV NO-DIM MB MB A0480 22 32 23.5 95. 2.5 A0480 22 33 23.5 97. 7.1 A0480 22 34 23.5 99. 1.4 A0480 22 35 23.5 103. 4.8 A0480 22 36 23.5 105. 3.3 A0480 22 37 23.5 111. 0.29 A0480 22 38 23.5 115. 3.4 A0480 22 39 23.5 139. 6.7 A0480 22 40 23.5 140. 5.9 A0480 22 41 23.5 141. 11. A0480 22 42 23.5 143. 10. A0480 22 43 23.5 144. 3.1 A0480 22 44 23.5 147. 2.1 A0480 22 45 23.5 157. 0.07 A0480 22 46 26.2 95. 12. A0480 22 47 26.2 97. 17. A0480 22 48 26.2 111. 11. A0480 22 49 26.2 115. 10. A0480 22 50 26.2 135. 4.0 A0480 22 51 26.2 139. 16. A0480 22 52 26.2 140. 17. A0480 22 53 27.8 95. 17. A0480 22 54 27.8 97. 17. A0480 22 55 27.8 115. 16. A0480 22 56 27.8 141. 29. A0480 22 57 27.8 143. 17. A0480 22 58 27.8 144. 14. A0480 22 59 27.8 147. 9.2 A0480 22 60 27.8 156. 2.4 A0480 22 61 27.8 157. 1.9 A0480 22 62 27.8 161. 0.77 A0480 22 63 30.7 95. 22. A0480 22 64 30.7 97. 14. A0480 22 65 30.7 115. 35. A0480 22 66 30.7 141. 15. A0480 22 67 30.7 143. 18. A0480 22 68 30.7 144. 18. A0480 22 69 35.3 89. 16. A0480 22 70 35.3 91. 21. A0480 22 71 35.3 95. 41. A0480 22 72 35.3 97. 44. A0480 22 73 35.3 103. 24. A0480 22 74 35.3 105. 28. A0480 22 75 35.3 106. 30. A0480 22 76 35.3 115. 44. A0480 22 77 35.3 135. 31. A0480 22 78 35.3 139. 37. A0480 22 79 35.3 140. 34. A0480 22 80 40.4 95. 48. A0480 22 81 40.4 97. 55. A0480 22 82 40.4 141. 46. A0480 22 83 40.4 144. 40. A0480 22 84 40.4 147. 22. A0480 22 85 40.4 156. 1.6 A0480 22 86 40.4 157. 1.8 A0480 22 87 40.4 161. 1.8 A0480 22 88 41.0 89. 10. A0480 22 89 41.0 91. 19. A0480 22 90 41.0 95. 44. A0480 22 91 41.0 97. 52. A0480 22 92 41.0 115. 47. A0480 22 93 41.0 135. 22. A0480 22 94 41.0 139. 31. A0480 22 95 41.0 140. 32. A0480 22 96 41.0 147. 4.4 A0480 22 97 44.3 89. 33. A0480 22 98 44.3 91. 58. A0480 22 99 44.3 95. 58. A0480 22 100 44.3 97. 53. A0480 22 101 44.3 99. 33. A0480 22 102 44.3 103. 28. A0480 22 103 44.3 105. 44. A0480 22 104 44.3 106. 51. A0480 22 105 44.3 111. 45. A0480 22 106 44.3 115. 74. A0480 22 107 44.3 135. 45. A0480 22 108 44.3 139. 55. A0480 22 109 44.3 140. 54. A0480 22 110 46.2 89. 22. A0480 22 111 46.2 91. 40. A0480 22 112 46.2 95. 61. A0480 22 113 46.2 97. 61. A0480 22 114 46.2 115. 82. A0480 22 115 46.2 135. 22. A0480 22 116 46.2 139. 83. A0480 22 117 46.2 140. 83. A0480 22 118 ENDDATA 88 0 A0480 22 119 ENDSUBENT 118 0 A0480 2299999 NOSUBENT A0480023 20200311 A094A0480 23 1 NOSUBENT A0480024 20200311 A094A0480 24 1 NOSUBENT A0480025 20200311 A094A0480 25 1 NOSUBENT A0480026 20200311 A094A0480 26 1 NOSUBENT A0480027 20200311 A094A0480 27 1 NOSUBENT A0480028 20200311 A094A0480 28 1 NOSUBENT A0480029 20200311 A094A0480 29 1 NOSUBENT A0480030 20200311 A094A0480 30 1 SUBENT A0480031 20200311 A094A0480 31 1 BIB 7 29 A0480 31 2 REACTION (92-U-235(A,F)MASS,CHN,SIG) A0480 31 3 SAMPLE The U-235 with isotopic purity > 99.9% used. Most of A0480 31 4 the targets were prepared by electrodeposition of 0.1 A0480 31 5 to 2 mg of hydrated uranium oxide over an area of aboutA0480 31 6 1 cm**2 on a dish-shaped aluminum disk. The amount of A0480 31 7 deposited material was determined by direct alpha A0480 31 8 counting, weighting, or both. These targets were then A0480 31 9 mounted in a water-cooled microtarget holder which alsoA0480 31 10 served as a Faraday cup for beam intensity measurementsA0480 31 11 ANALYSIS (CHGDS) A0480 31 12 ERR-ANALYS (DATA-ERR,15.,25.) These errors arise from many sourcesA0480 31 13 and are rather difficult to evaluate, The most likely A0480 31 14 source's of error are in the determination of the A0480 31 15 number of atoms per cm2 in the target, from A0480 31 16 uncertainties in decay schemes and counting correctionsA0480 31 17 of the observed products, and, to a lesser extent, A0480 31 18 uncertainties in mass chain yield corrections. A0480 31 19 FLAG (1.) Mass yield had been measured for 112-Pd. A0480 31 20 (2.) Mass yield had been measured for 112-Ag. A0480 31 21 (3.) Mass yield had been measured for 143-Pr. A0480 31 22 (4.) Mass yield had been measured for 143-Ce. A0480 31 23 STATUS (TABLE) Tbl. II of UCRL-3858,1957 report; partly given A0480 31 24 in Tbl. VI of Phys.Rev.,111(1958)1358 A0480 31 25 HISTORY (20160317A) SD: SF5=CUM -> CHN in REACTION code. A0480 31 26 ANALYSIS added. A0480 31 27 (20200311A) SD: Data from Subents 032-039 were added. A0480 31 28 STATUS updated. Several values corrected. Data from A0480 31 29 Tbl. II of UCRL-3858 report were added; several values A0480 31 30 corrected. A0480 31 31 ENDBIB 29 0 A0480 31 32 NOCOMMON 0 0 A0480 31 33 DATA 4 134 A0480 31 34 EN MASS DATA FLAG A0480 31 35 MEV NO-DIM MB NO-DIM A0480 31 36 18.7 89. 0.098 A0480 31 37 18.7 91. 0.097 A0480 31 38 18.7 97. 0.075 A0480 31 39 18.7 105. 0.017 A0480 31 40 18.7 139. 0.11 A0480 31 41 18.7 140. 0.13 A0480 31 42 21.9 95. 4.24 A0480 31 43 21.9 97. 4.5 A0480 31 44 21.9 115. 0.87 A0480 31 45 21.9 117. 0.94 A0480 31 46 21.9 141. 2.1 A0480 31 47 21.9 143. 1.6 A0480 31 48 21.9 144. 1.1 A0480 31 49 23.6 72. 0.30 A0480 31 50 23.6 95. 8.6 A0480 31 51 23.6 97. 9.5 A0480 31 52 23.6 115. 3.55 A0480 31 53 25.2 115. 5.9 A0480 31 54 25.2 117. 5.3 A0480 31 55 25.2 141. 6.3 A0480 31 56 25.2 143. 4.5 4. A0480 31 57 25.2 143. 3.7 3. A0480 31 58 25.2 144. 3.2 A0480 31 59 26.8 89. 10.2 A0480 31 60 26.8 91. 11.2 A0480 31 61 26.8 95. 16.5 A0480 31 62 26.8 97. 17.6 A0480 31 63 26.8 99. 18.6 A0480 31 64 26.8 103. 11.9 A0480 31 65 26.8 105. 11.5 A0480 31 66 26.8 106. 11.5 A0480 31 67 26.8 111. 11.0 A0480 31 68 26.8 112. 10.1 A0480 31 69 26.8 113. 11.2 A0480 31 70 26.8 115. 11.7 A0480 31 71 26.8 139. 19.4 A0480 31 72 26.8 140. 15.4 A0480 31 73 26.8 141. 13.9 A0480 31 74 26.8 143. 12.8 A0480 31 75 26.8 144. 8.9 A0480 31 76 26.8 147. 7.5 A0480 31 77 26.8 156. 0.63 A0480 31 78 26.8 157. 0.73 A0480 31 79 26.8 159. 0.35 A0480 31 80 27.3 95. 17.5 A0480 31 81 27.3 97. 22.5 A0480 31 82 27.3 115. 10.1 A0480 31 83 27.3 117. 10.3 A0480 31 84 29.7 95. 29.0 A0480 31 85 29.7 97. 30.0 A0480 31 86 29.7 115. 13.9 A0480 31 87 29.7 117. 10.3 A0480 31 88 30.6 89. 17.2 A0480 31 89 30.6 91. 18.3 A0480 31 90 30.6 95. 30.0 A0480 31 91 30.6 97. 33.0 A0480 31 92 30.6 115. 18.5 A0480 31 93 30.6 117. 16.2 A0480 31 94 30.6 139. 26.1 A0480 31 95 30.6 140. 24.0 A0480 31 96 32.8 89. 21.9 A0480 31 97 32.8 91. 24.5 A0480 31 98 32.8 95. 32.0 A0480 31 99 32.8 97. 32.8 A0480 31 100 32.8 99. 35.1 A0480 31 101 32.8 111. 33.4 A0480 31 102 32.8 112. 32.6 A0480 31 103 32.8 115. 36.7 A0480 31 104 32.8 140. 36.1 A0480 31 105 32.8 141. 27.8 A0480 31 106 32.8 143. 39.2 A0480 31 107 32.8 144. 22.7 A0480 31 108 32.8 147. 15.9 A0480 31 109 32.8 156. 2.6 A0480 31 110 32.8 157. 2.8 A0480 31 111 32.8 159. 0.82 A0480 31 112 34.1 89. 23.0 A0480 31 113 34.1 91. 27.4 A0480 31 114 34.1 95. 39.6 A0480 31 115 34.1 97. 45.4 A0480 31 116 34.1 115. 39.6 A0480 31 117 34.1 117. 38.3 A0480 31 118 34.1 139. 42.3 A0480 31 119 34.1 140. 40.8 A0480 31 120 34.1 141. 52.0 A0480 31 121 34.1 143. 33.8 A0480 31 122 34.1 144. 21.6 A0480 31 123 34.1 147. 22.2 A0480 31 124 34.1 156. 4.93 A0480 31 125 34.1 157. 4.26 A0480 31 126 34.1 161. 0.49 A0480 31 127 37.1 89. 26.7 A0480 31 128 37.1 91. 29.0 A0480 31 129 37.1 95. 47.7 A0480 31 130 37.1 97. 52.9 A0480 31 131 37.1 115. 49.0 A0480 31 132 37.1 117. 49.0 A0480 31 133 37.1 139. 40.3 A0480 31 134 37.1 140. 39.5 A0480 31 135 39.5 95. 53.7 A0480 31 136 39.5 97. 60.8 A0480 31 137 39.5 115. 57.9 A0480 31 138 42.8 72. 0.52 A0480 31 139 42.8 95. 50.6 A0480 31 140 42.8 97. 56.5 A0480 31 141 42.8 115. 53.1 A0480 31 142 42.8 117. 65.5 A0480 31 143 45. 89. 60.4 A0480 31 144 45. 91. 59.2 A0480 31 145 45. 95. 47.2 A0480 31 146 45. 97. 62.9 A0480 31 147 45. 99. 63.7 A0480 31 148 45. 103. 52.0 A0480 31 149 45. 105. 53.2 A0480 31 150 45. 106. 64.1 A0480 31 151 45. 111. 71.7 A0480 31 152 45. 112. 54.0 1. A0480 31 153 45. 112. 54.0 2. A0480 31 154 45. 113. 79.8 A0480 31 155 45. 115. 62.1 A0480 31 156 45. 140. 62.9 A0480 31 157 45. 141. 41.5 A0480 31 158 45. 143. 41.1 A0480 31 159 45. 144. 33.9 A0480 31 160 45. 147. 19.1 A0480 31 161 45. 156. 3.67 A0480 31 162 45. 157. 3.71 A0480 31 163 45. 159. 2.3 A0480 31 164 45. 161. 1.0 A0480 31 165 45.5 72. 0.65 A0480 31 166 45.5 95. 59.0 A0480 31 167 45.5 97. 59.2 A0480 31 168 45.5 115. 75.4 A0480 31 169 45.5 140. 44.0 A0480 31 170 ENDDATA 136 0 A0480 31 171 ENDSUBENT 170 0 A0480 3199999 NOSUBENT A0480032 20200311 A094A0480 32 1 NOSUBENT A0480033 20200311 A094A0480 33 1 NOSUBENT A0480034 20200311 A094A0480 34 1 NOSUBENT A0480035 20200311 A094A0480 35 1 NOSUBENT A0480036 20200311 A094A0480 36 1 NOSUBENT A0480037 20200311 A094A0480 37 1 NOSUBENT A0480038 20200311 A094A0480 38 1 NOSUBENT A0480039 20200311 A094A0480 39 1 SUBENT A0480040 20231226 A105A0480 40 1 BIB 7 24 A0480 40 2 REACTION (92-U-238(A,F)MASS,CHN,SIG) A0480 40 3 SAMPLE The U-238 with isotopic purity > 99.% used. Most of A0480 40 4 the targets were prepared by electrodeposition of 0.1 A0480 40 5 to 2 mg of hydrated uranium oxide over an area of aboutA0480 40 6 1 cm**2 on a dish-shaped aluminum disk. The amount of A0480 40 7 deposited material was determined by direct alpha A0480 40 8 counting, weighting, or both. These targets were then A0480 40 9 mounted in a water-cooled microtarget holder which alsoA0480 40 10 served as a Faraday cup for beam intensity measurementsA0480 40 11 ANALYSIS (CHGDS) A0480 40 12 ERR-ANALYS (DATA-ERR) The limits of error are estimated to be A0480 40 13 about 15% for most of the mass chains reported. A0480 40 14 However, at higher energies, the chain yield A0480 40 15 corrections become quite sizeable and the errors A0480 40 16 may be somewhat greater. A0480 40 17 FLAG (2.) Cross section is for 129m-Te only. A0480 40 18 (1.) Cross section is approximated owing to A0480 40 19 complexities in the decay scheme. A0480 40 20 STATUS (TABLE,,R.Vandenbosch+,J,PR,111,1358,1958) Tbl. VII A0480 40 21 HISTORY (20160317A) SD: SF5=CUM -> CHN in REACTION code. A0480 40 22 ANALYSIS added. A0480 40 23 (20200311A) SD: Data from Subents 041-048 were added. A0480 40 24 STATUS updated. Several values corrected. A0480 40 25 (20231226A) SD: Col.EN deleted from COMMON section. A0480 40 26 ENDBIB 24 0 A0480 40 27 COMMON 1 3 A0480 40 28 DATA-ERR A0480 40 29 PER-CENT A0480 40 30 15. A0480 40 31 ENDCOMMON 3 0 A0480 40 32 DATA 4 72 A0480 40 33 EN MASS DATA FLAG A0480 40 34 MEV NO-DIM MB NO-DIM A0480 40 35 22.6 95. 4.7 A0480 40 36 22.6 97. 8.2 A0480 40 37 22.6 103. 6.5 A0480 40 38 22.6 105. 7.0 A0480 40 39 22.6 115. 2.6 A0480 40 40 22.6 117. 2.0 A0480 40 41 22.6 139. 7.0 A0480 40 42 22.6 140. 6.7 A0480 40 43 25.2 143. 12.1 A0480 40 44 27.1 95. 29. A0480 40 45 27.1 97. 37. A0480 40 46 27.1 115. 15.4 A0480 40 47 27.1 141. 40. A0480 40 48 27.1 143. 24. A0480 40 49 27.1 147. 15.4 A0480 40 50 27.1 156. 1.9 A0480 40 51 27.1 157. 1.7 A0480 40 52 27.1 161. 0.31 A0480 40 53 32.5 95. 21. A0480 40 54 32.5 97. 35. A0480 40 55 33.8 95. 28. A0480 40 56 33.8 97. 42. A0480 40 57 33.8 140. 36. A0480 40 58 38.6 95. 38. A0480 40 59 38.6 97. 56. A0480 40 60 38.6 103. 47. A0480 40 61 38.6 105. 36. A0480 40 62 38.6 115. 48. A0480 40 63 38.6 139. 41. A0480 40 64 38.6 140. 43. A0480 40 65 38.6 143. 48. A0480 40 66 38.6 147. 28. A0480 40 67 38.6 156. 3.7 A0480 40 68 38.6 157. 2.8 A0480 40 69 38.6 161. 0.48 A0480 40 70 40. 89. 24. A0480 40 71 40. 91. 28. A0480 40 72 40. 95. 35. A0480 40 73 40. 97. 56. A0480 40 74 40. 99. 59. A0480 40 75 40. 103. 44. A0480 40 76 40. 105. 53. A0480 40 77 40. 111. 43. A0480 40 78 40. 112. 56. A0480 40 79 40. 113. 49. A0480 40 80 40. 115. 60. A0480 40 81 40. 129. 35. 2. A0480 40 82 40. 132. 74. 1. A0480 40 83 40. 140. 43. A0480 40 84 40. 143. 52. A0480 40 85 40. 147. 20. A0480 40 86 40. 156. 4.5 A0480 40 87 40. 157. 2.5 A0480 40 88 40. 159. 0.71 A0480 40 89 43.9 95. 41. A0480 40 90 43.9 97. 56. A0480 40 91 43.9 103. 51. A0480 40 92 43.9 105. 55. A0480 40 93 43.9 115. 58. A0480 40 94 43.9 117. 64. 1. A0480 40 95 43.9 139. 45. A0480 40 96 43.9 140. 50. A0480 40 97 43.9 143. 33. A0480 40 98 45.4 89. 27. A0480 40 99 45.4 91. 36. A0480 40 100 45.4 95. 36. A0480 40 101 45.4 97. 54. A0480 40 102 45.4 103. 47. A0480 40 103 45.4 105. 48. A0480 40 104 45.4 115. 49. A0480 40 105 45.4 139. 51. A0480 40 106 45.4 140. 50. A0480 40 107 ENDDATA 74 0 A0480 40 108 ENDSUBENT 107 0 A0480 4099999 NOSUBENT A0480041 20200311 A094A0480 41 1 NOSUBENT A0480042 20200311 A094A0480 42 1 NOSUBENT A0480043 20200311 A094A0480 43 1 NOSUBENT A0480044 20200311 A094A0480 44 1 NOSUBENT A0480045 20200311 A094A0480 45 1 NOSUBENT A0480046 20200311 A094A0480 46 1 NOSUBENT A0480047 20200311 A094A0480 47 1 NOSUBENT A0480048 20200311 A094A0480 48 1 SUBENT A0480049 20200311 A094A0480 49 1 BIB 5 13 A0480 49 2 REACTION (93-NP-237(D,2N)94-PU-237,,SIG) A0480 49 3 SAMPLE Most of the neptunium targets were prepared in the sameA0480 49 4 manner as the uranium targets. The plating yields of A0480 49 5 neptunium were quite low; a modified procedure using a A0480 49 6 solution of 0.15 M ammonium formate and 0.2 M A0480 49 7 perchloric acid was found to give somewhat better A0480 49 8 yields. The amount of material deposited was determinedA0480 49 9 by alpha counting and also checked occasionally by A0480 49 10 assaying the target solution after the target A0480 49 11 had been bombarded and dissolved. A0480 49 12 STATUS (TABLE) Tbl. IV from UCRL-3858,1057 report. A0480 49 13 ERR-ANALYS (DATA-ERR) No information about source of uncertainty A0480 49 14 HISTORY (20200311C) SD A0480 49 15 ENDBIB 13 0 A0480 49 16 COMMON 1 3 A0480 49 17 DATA-ERR A0480 49 18 PER-CENT A0480 49 19 15. A0480 49 20 ENDCOMMON 3 0 A0480 49 21 DATA 2 6 A0480 49 22 EN DATA A0480 49 23 MEV MB A0480 49 24 13.7 13.2 A0480 49 25 16.0 15.6 A0480 49 26 18.3 14.2 A0480 49 27 20.6 12.0 A0480 49 28 22.0 11.3 A0480 49 29 23.3 12.5 A0480 49 30 ENDDATA 8 0 A0480 49 31 ENDSUBENT 30 0 A0480 4999999 SUBENT A0480050 20200311 A094A0480 50 1 BIB 5 13 A0480 50 2 REACTION (93-NP-237(D,3N)94-PU-236,,SIG) A0480 50 3 SAMPLE Most of the neptunium targets were prepared in the sameA0480 50 4 manner as the uranium targets. The plating yields of A0480 50 5 neptunium were quite low; a modified procedure using a A0480 50 6 solution of 0.15 M ammonium formate and 0.2 M A0480 50 7 perchloric acid was found to give somewhat better A0480 50 8 yields. The amount of material deposited was determinedA0480 50 9 by alpha counting and also checked occasionally by A0480 50 10 assaying the target solution after the target A0480 50 11 had been bombarded and dissolved. A0480 50 12 STATUS (TABLE) Tbl. IV from UCRL-3858,1057 report. A0480 50 13 ERR-ANALYS (DATA-ERR) No information about source of uncertainty A0480 50 14 HISTORY (20200311C) SD A0480 50 15 ENDBIB 13 0 A0480 50 16 COMMON 1 3 A0480 50 17 DATA-ERR A0480 50 18 PER-CENT A0480 50 19 15. A0480 50 20 ENDCOMMON 3 0 A0480 50 21 DATA 2 6 A0480 50 22 EN DATA A0480 50 23 MEV MB A0480 50 24 13.7 2.16 A0480 50 25 16.0 10. A0480 50 26 18.3 13.6 A0480 50 27 20.6 9.2 A0480 50 28 22.0 7.8 A0480 50 29 23.3 7.6 A0480 50 30 ENDDATA 8 0 A0480 50 31 ENDSUBENT 30 0 A0480 5099999 SUBENT A0480051 20200311 A094A0480 51 1 BIB 5 13 A0480 51 2 REACTION (93-NP-237(D,P)93-NP-238,,SIG) A0480 51 3 SAMPLE Most of the neptunium targets were prepared in the sameA0480 51 4 manner as the uranium targets. The plating yields of A0480 51 5 neptunium were quite low; a modified procedure using a A0480 51 6 solution of 0.15 M ammonium formate and 0.2 M A0480 51 7 perchloric acid was found to give somewhat better A0480 51 8 yields. The amount of material deposited was determinedA0480 51 9 by alpha counting and also checked occasionally by A0480 51 10 assaying the target solution after the target A0480 51 11 had been bombarded and dissolved. A0480 51 12 STATUS (TABLE) Tbl. IV from UCRL-3858,1057 report. A0480 51 13 ERR-ANALYS (DATA-ERR) No information about source of uncertainty A0480 51 14 HISTORY (20200311C) SD A0480 51 15 ENDBIB 13 0 A0480 51 16 COMMON 1 3 A0480 51 17 DATA-ERR A0480 51 18 PER-CENT A0480 51 19 15. A0480 51 20 ENDCOMMON 3 0 A0480 51 21 DATA 2 12 A0480 51 22 EN DATA A0480 51 23 MEV MB A0480 51 24 8.6 23. A0480 51 25 11.9 67. A0480 51 26 13.9 80. A0480 51 27 15.8 73. A0480 51 28 16.0 177. A0480 51 29 18.3 146. A0480 51 30 18.4 126. A0480 51 31 20.6 117. A0480 51 32 21.7 88. A0480 51 33 22.0 99. A0480 51 34 22.0 107. A0480 51 35 23.3 93. A0480 51 36 ENDDATA 14 0 A0480 51 37 ENDSUBENT 36 0 A0480 5199999 SUBENT A0480052 20200311 A094A0480 52 1 BIB 5 13 A0480 52 2 REACTION (93-NP-237(D,P)93-NP-238,,SIG) A0480 52 3 SAMPLE Most of the neptunium targets were prepared in the sameA0480 52 4 manner as the uranium targets. The plating yields of A0480 52 5 neptunium were quite low; a modified procedure using a A0480 52 6 solution of 0.15 M ammonium formate and 0.2 M A0480 52 7 perchloric acid was found to give somewhat better A0480 52 8 yields. The amount of material deposited was determinedA0480 52 9 by alpha counting and also checked occasionally by A0480 52 10 assaying the target solution after the target A0480 52 11 had been bombarded and dissolved. A0480 52 12 STATUS (TABLE) Tbl. IV from UCRL-3858,1057 report. A0480 52 13 ERR-ANALYS (DATA-ERR) No information about source of uncertainty A0480 52 14 HISTORY (20200311C) SD A0480 52 15 ENDBIB 13 0 A0480 52 16 COMMON 1 3 A0480 52 17 DATA-ERR A0480 52 18 PER-CENT A0480 52 19 15. A0480 52 20 ENDCOMMON 3 0 A0480 52 21 DATA 2 14 A0480 52 22 EN DATA A0480 52 23 MEV MB A0480 52 24 8.6 0.24 A0480 52 25 11.9 5.2 A0480 52 26 13.7 26. A0480 52 27 13.9 14.3 A0480 52 28 15.8 16.5 A0480 52 29 16.0 36.5 A0480 52 30 18.3 42.0 A0480 52 31 18.4 37.2 A0480 52 32 20.6 38.5 A0480 52 33 21.7 32.7 A0480 52 34 22.0 36.0 A0480 52 35 22.0 41.5 A0480 52 36 23.3 39.5 A0480 52 37 23.3 46.0 A0480 52 38 ENDDATA 16 0 A0480 52 39 ENDSUBENT 38 0 A0480 5299999 SUBENT A0480053 20200311 A094A0480 53 1 BIB 5 17 A0480 53 2 REACTION (92-U-233(A,F)ELEM/MASS,CUM,SIG) A0480 53 3 SAMPLE The U-233 (isotopic purity of approximately 96%, A0480 53 4 U-238 - 3%, U-234 <1%). Most of the targets were A0480 53 5 prepared by electrodeposition of 0.1 to 2 mg of A0480 53 6 hydrated uranium oxide over an area of about 1 cm**2 onA0480 53 7 a dish-shaped aluminum disk. The amount of deposited A0480 53 8 material was determined by direct alpha counting, A0480 53 9 weighting, or both. These targets were then mounted in A0480 53 10 a water-cooled micro-target holder which also served asA0480 53 11 a Faraday cup for beam intensity measurements. A0480 53 12 ERR-ANALYS (DATA-ERR) The limits of error are estimated to be A0480 53 13 about 15% for most of the mass chains reported. A0480 53 14 However, at higher energies, the chain yield A0480 53 15 corrections become quite sizeable and the errors A0480 53 16 may be somewhat greater. A0480 53 17 STATUS (TABLE) Tbl. V from Phys.Rev.,111(1958)1358 A0480 53 18 HISTORY (20200311C) SD A0480 53 19 ENDBIB 17 0 A0480 53 20 COMMON 1 3 A0480 53 21 DATA-ERR A0480 53 22 PER-CENT A0480 53 23 15. A0480 53 24 ENDCOMMON 3 0 A0480 53 25 DATA 6 86 A0480 53 26 EN ELEMENT MASS ISOMER DATA DATA-MIN A0480 53 27 MEV NO-DIM NO-DIM NO-DIM MB MB A0480 53 28 23.5 40. 95. 2.4 A0480 53 29 23.5 40. 97. 6.5 A0480 53 30 23.5 42. 99. 1.4 A0480 53 31 23.5 44. 103. 4.8 A0480 53 32 23.5 44. 105. 3.2 A0480 53 33 23.5 47. 111. 0.29A0480 53 34 23.5 48. 115. 3.3 A0480 53 35 23.5 56. 139. 4.6 A0480 53 36 23.5 56. 140. 3.4 A0480 53 37 23.5 58. 141. 10. A0480 53 38 23.5 58. 143. 8.4 A0480 53 39 23.5 58. 144. 2.1 A0480 53 40 23.5 60. 147. 2.0 A0480 53 41 23.5 63. 157. 0.04 A0480 53 42 26.2 40. 95. 12. A0480 53 43 26.2 40. 97. 15. A0480 53 44 26.2 47. 111. 11. A0480 53 45 26.2 48. 115. 9.9 A0480 53 46 26.2 56. 135. 1.0 0.42 A0480 53 47 26.2 56. 139. 9.2 A0480 53 48 26.2 56. 140. 7.4 A0480 53 49 27.8 40. 95. 17. A0480 53 50 27.8 40. 97. 15. A0480 53 51 27.8 48. 115. 15. A0480 53 52 27.8 58. 141. 26. A0480 53 53 27.8 58. 143. 13. A0480 53 54 27.8 58. 144. 8.0 A0480 53 55 27.8 60. 147. 8.0 A0480 53 56 27.8 63. 156. 0.68 A0480 53 57 27.8 63. 157. 0.94 A0480 53 58 27.8 65. 161. 0.50 A0480 53 59 30.7 40. 95. 21. A0480 53 60 30.7 40. 97. 12. A0480 53 61 30.7 48. 115. 32. A0480 53 62 30.7 58. 141. 13. A0480 53 63 30.7 58. 143. 12. A0480 53 64 30.7 58. 144. 8.8 A0480 53 65 35.3 38. 89. 16. A0480 53 66 35.3 38. 91. 19. A0480 53 67 35.3 40. 95. 39. A0480 53 68 35.3 40. 97. 38. A0480 53 69 35.3 44. 103. 24. A0480 53 70 35.3 44. 105. 27. A0480 53 71 35.3 44. 106. 27. A0480 53 72 35.3 48. 115. 41. A0480 53 73 35.3 56. 135. 1. 4.9 A0480 53 74 35.3 56. 139. 18. A0480 53 75 35.3 56. 140. 12. A0480 53 76 40.4 40. 95. 46. A0480 53 77 40.4 40. 97. 45. A0480 53 78 40.4 58. 141. 39. A0480 53 79 40.4 58. 144. 15. A0480 53 80 40.4 60. 147. 15. A0480 53 81 40.4 63. 156. 0.44 A0480 53 82 40.4 63. 157. 0.48 A0480 53 83 40.4 65. 161. 0.71 A0480 53 84 41.0 38. 89. 9.9 A0480 53 85 41.0 38. 91. 17. A0480 53 86 41.0 40. 95. 42. A0480 53 87 41.0 40. 97. 44. A0480 53 88 41.0 48. 115. 43. A0480 53 89 41.0 56. 135. 1. 4.0 A0480 53 90 41.0 56. 139. 12. A0480 53 91 41.0 56. 140. 8.4 A0480 53 92 41.0 60. 147. 3.0 A0480 53 93 44.3 38. 89. 32. A0480 53 94 44.3 38. 91. 52. A0480 53 95 44.3 40. 95. 55. A0480 53 96 44.3 40. 97. 43. A0480 53 97 44.3 42. 99. 32. A0480 53 98 44.3 44. 103. 28. A0480 53 99 44.3 44. 105. 41. A0480 53 100 44.3 44. 106. 45. A0480 53 101 44.3 47. 111. 44.A0480 53 102 44.3 48. 115. 68. A0480 53 103 44.3 56. 135. 1. 8.5 A0480 53 104 44.3 56. 139. 22. A0480 53 105 44.3 56. 140. 14. A0480 53 106 46.2 38. 89. 22. A0480 53 107 46.2 38. 91. 35. A0480 53 108 46.2 40. 95. 57. A0480 53 109 46.2 40. 97. 48. A0480 53 110 46.2 48. 115. 74. A0480 53 111 46.2 56. 135. 1. 4.9 A0480 53 112 46.2 56. 139. 25. A0480 53 113 46.2 56. 140. 16. A0480 53 114 ENDDATA 88 0 A0480 53 115 ENDSUBENT 114 0 A0480 5399999 SUBENT A0480054 20200311 A094A0480 54 1 BIB 6 18 A0480 54 2 REACTION (92-U-235(A,F)ELEM/MASS,CUM,SIG) A0480 54 3 SAMPLE The U-235 with isotopic purity > 99.9% used. Most of A0480 54 4 the targets were prepared by electrodeposition of 0.1 A0480 54 5 to 2 mg of hydrated uranium oxide over an area of aboutA0480 54 6 1 cm**2 on a dish-shaped aluminum disk. The amount of A0480 54 7 deposited material was determined by direct alpha A0480 54 8 counting, weighting, or both. These targets were then A0480 54 9 mounted in a water-cooled microtarget holder which alsoA0480 54 10 served as a Faraday cup for beam intensity measurementsA0480 54 11 ANALYSIS (CHGDS) A0480 54 12 ERR-ANALYS (DATA-ERR) The limits of error are estimated to be A0480 54 13 about 15% for most of the mass chains reported. A0480 54 14 However, at higher energies, the chain yield A0480 54 15 corrections become quite sizeable and the errors A0480 54 16 may be somewhat greater. A0480 54 17 STATUS (TABLE) Tbl. II of UCRL-3858,1957 report; partly given A0480 54 18 in Tbl. VI of Phys.Rev.,111(1958)1358 A0480 54 19 HISTORY (20200311C) SD A0480 54 20 ENDBIB 18 0 A0480 54 21 COMMON 1 3 A0480 54 22 DATA-ERR A0480 54 23 PER-CENT A0480 54 24 15. A0480 54 25 ENDCOMMON 3 0 A0480 54 26 DATA 5 162 A0480 54 27 EN ELEMENT MASS ISOMER DATA A0480 54 28 MEV NO-DIM NO-DIM NO-DIM MB A0480 54 29 18.7 38. 89. 0.098 A0480 54 30 18.7 38. 91. 0.095 A0480 54 31 18.7 40. 97. 0.071 A0480 54 32 18.7 44. 105. 0.017 A0480 54 33 18.7 56. 139. 0.10 A0480 54 34 18.7 56. 140. 0.10 A0480 54 35 21.9 40. 95. 4.24 A0480 54 36 21.9 40. 97. 4.3 A0480 54 37 21.9 48. 115. 1. 0.073 A0480 54 38 21.9 48. 115. 0. 0.80 A0480 54 39 21.9 48. 115. 0.87 A0480 54 40 21.9 48. 117. 0.90 A0480 54 41 21.9 58. 141. 2.1 A0480 54 42 21.9 58. 143. 1.5 A0480 54 43 21.9 58. 144. 0.98 A0480 54 44 23.6 35. 72. 0.30 A0480 54 45 23.6 40. 95. 8.53 A0480 54 46 23.6 40. 97. 9.05 A0480 54 47 23.6 48. 115. 1. 0.25 A0480 54 48 23.6 48. 115. 0. 3.27 A0480 54 49 23.6 48. 115. 3.52 A0480 54 50 25.2 48. 115. 1. 0.423 A0480 54 51 25.2 48. 115. 0. 5.43 A0480 54 52 25.2 48. 115. 5.85 A0480 54 53 25.2 48. 117. 5.0 A0480 54 54 25.2 58. 141. 6.1 A0480 54 55 25.2 58. 143. 4.1 A0480 54 56 25.2 58. 144. 2.9 A0480 54 57 25.2 59. 143. 3.33 A0480 54 58 26.8 38. 89. 10.2 A0480 54 59 26.8 38. 91. 11.0 A0480 54 60 26.8 40. 95. 16.4 A0480 54 61 26.8 40. 97. 16.8 A0480 54 62 26.8 42. 99. 18.6 A0480 54 63 26.8 44. 103. 11.9 A0480 54 64 26.8 44. 105. 11.5 A0480 54 65 26.8 44. 106. 11.2 A0480 54 66 26.8 46. 112. 9.7 A0480 54 67 26.8 47. 111. 11.0 A0480 54 68 26.8 47. 113. 11.1 A0480 54 69 26.8 48. 115. 1. 1.29 A0480 54 70 26.8 48. 115. 0. 10.3 A0480 54 71 26.8 48. 115. 11.6 A0480 54 72 26.8 56. 139. 16.2 A0480 54 73 26.8 56. 140. 10.9 A0480 54 74 26.8 58. 141. 13.6 A0480 54 75 26.8 58. 143. 11.5 A0480 54 76 26.8 58. 144. 7.4 A0480 54 77 26.8 60. 147. 7.1 A0480 54 78 26.8 63. 156. 0.55 A0480 54 79 26.8 63. 157. 0.57 A0480 54 80 26.8 64. 159. 0.29 A0480 54 81 27.3 40. 95. 17.2 A0480 54 82 27.3 40. 97. 20.9 A0480 54 83 27.3 48. 115. 1. 1.0 A0480 54 84 27.3 48. 115. 0. 9.06 A0480 54 85 27.3 48. 115. 10.1 A0480 54 86 27.3 48. 117. 9.56 A0480 54 87 29.7 40. 95. 28.6 A0480 54 88 29.7 40. 97. 27.8 A0480 54 89 29.7 48. 115. 1. 1.2 A0480 54 90 29.7 48. 115. 0. 12.5 A0480 54 91 29.7 48. 115. 13.7 A0480 54 92 29.7 48. 117. 9.55 A0480 54 93 30.6 38. 89. 17.2 A0480 54 94 30.6 38. 91. 17.6 A0480 54 95 30.6 40. 95. 29.3 A0480 54 96 30.6 40. 97. 30.6 A0480 54 97 30.6 48. 115. 1. 1.65 A0480 54 98 30.6 48. 115. 0. 16.6 A0480 54 99 30.6 48. 115. 18.2 A0480 54 100 30.6 48. 117. 15.0 A0480 54 101 30.6 56. 139. 20.1 A0480 54 102 30.6 56. 140. 15.3 A0480 54 103 32.8 38. 89. 21.9 A0480 54 104 32.8 38. 91. 23.6 A0480 54 105 32.8 40. 95. 31.8 A0480 54 106 32.8 40. 97. 30.7 A0480 54 107 32.8 42. 99. 35.1 A0480 54 108 32.8 46. 112. 30.4 A0480 54 109 32.8 47. 111. 33.4 A0480 54 110 32.8 48. 115. 1. 3.7 A0480 54 111 32.8 48. 115. 0. 32.7 A0480 54 112 32.8 48. 115. 36.4 A0480 54 113 32.8 56. 140. 22.6 A0480 54 114 32.8 58. 141. 27.6 A0480 54 115 32.8 58. 143. 34.4 A0480 54 116 32.8 58. 144. 17.5 A0480 54 117 32.8 60. 147. 14.7 A0480 54 118 32.8 63. 156. 2.1 A0480 54 119 32.8 63. 157. 1.94 A0480 54 120 32.8 64. 159. 0.55 A0480 54 121 34.1 38. 89. 22.9 A0480 54 122 34.1 38. 91. 26.0 A0480 54 123 34.1 40. 95. 38.8 A0480 54 124 34.1 40. 97. 41.8 A0480 54 125 34.1 48. 115. 1. 3.17 A0480 54 126 34.1 48. 115. 0. 35.2 A0480 54 127 34.1 48. 115. 38.4 A0480 54 128 34.1 48. 117. 34.8 A0480 54 129 34.1 56. 139. 29.5 A0480 54 130 34.1 56. 140. 22.0 A0480 54 131 34.1 58. 141. 49.0 A0480 54 132 34.1 58. 143. 27.0 A0480 54 133 34.1 58. 144. 14.9 A0480 54 134 34.1 60. 147. 19.8 A0480 54 135 34.1 63. 156. 3.64 A0480 54 136 34.1 63. 157. 2.68 A0480 54 137 34.1 65. 161. 0.36 A0480 54 138 37.1 38. 89. 26.5 A0480 54 139 37.1 38. 91. 27.6 A0480 54 140 37.1 40. 95. 46.7 A0480 54 141 37.1 40. 97. 48.7 A0480 54 142 37.1 48. 115. 1. 3.86 A0480 54 143 37.1 48. 115. 0. 43.8 A0480 54 144 37.1 48. 115. 47.7 A0480 54 145 37.1 48. 117. 44.6 A0480 54 146 37.1 56. 139. 29.9 A0480 54 147 37.1 56. 140. 21.3 A0480 54 148 39.5 40. 95. 52.1 A0480 54 149 39.5 40. 97. 54.1 A0480 54 150 39.5 48. 115. 1. 4.3 A0480 54 151 39.5 48. 115. 0. 51.3 A0480 54 152 39.5 48. 115. 55.6 A0480 54 153 42.8 35. 72. 0.48 A0480 54 154 42.8 40. 95. 49.1 A0480 54 155 42.8 40. 97. 50.3 A0480 54 156 42.8 48. 115. 1. 4.4 A0480 54 157 42.8 48. 115. 0. 46.5 A0480 54 158 42.8 48. 115. 50.9 A0480 54 159 42.8 48. 117. 57.0 A0480 54 160 45. 38. 89. 59.6 A0480 54 161 45. 38. 91. 55.6 A0480 54 162 45. 40. 95. 45.5 A0480 54 163 45. 40. 97. 55.6 A0480 54 164 45. 42. 99. 62.9 A0480 54 165 45. 44. 103. 52.0 A0480 54 166 45. 44. 105. 51.6 A0480 54 167 45. 44. 106. 60.0 A0480 54 168 45. 46. 112. 47.6 A0480 54 169 45. 47. 111. 71.7 A0480 54 170 45. 47. 112. 47.6 A0480 54 171 45. 47. 113. 75.7 A0480 54 172 45. 48. 115. 1. 10.1 A0480 54 173 45. 48. 115. 0. 49.6 A0480 54 174 45. 48. 115. 59.7 A0480 54 175 45. 56. 140. 29.0 A0480 54 176 45. 58. 141. 38.1 A0480 54 177 45. 58. 143. 30.6 A0480 54 178 45. 58. 144. 20.4 A0480 54 179 45. 60. 147. 16.0 A0480 54 180 45. 63. 156. 2.38 A0480 54 181 45. 63. 157. 1.83 A0480 54 182 45. 64. 159. 1.3 A0480 54 183 45. 65. 161. 0.67 A0480 54 184 45.5 35. 72. 0.60 A0480 54 185 45.5 40. 95. 57.2 A0480 54 186 45.5 40. 97. 52.7 A0480 54 187 45.5 48. 115. 1. 10.9 A0480 54 188 45.5 48. 115. 0. 61.5 A0480 54 189 45.5 48. 115. 72.4 A0480 54 190 45.5 56. 140. 20.2 A0480 54 191 ENDDATA 164 0 A0480 54 192 ENDSUBENT 191 0 A0480 5499999 SUBENT A0480055 20200311 A094A0480 55 1 BIB 6 17 A0480 55 2 REACTION (92-U-238(A,F)ELEM/MASS,CUM,SIG) A0480 55 3 SAMPLE The U-238 with isotopic purity > 99.% used. Most of A0480 55 4 the targets were prepared by electrodeposition of 0.1 A0480 55 5 to 2 mg of hydrated uranium oxide over an area of aboutA0480 55 6 1 cm**2 on a dish-shaped aluminum disk. The amount of A0480 55 7 deposited material was determined by direct alpha A0480 55 8 counting, weighting, or both. These targets were then A0480 55 9 mounted in a water-cooled microtarget holder which alsoA0480 55 10 served as a Faraday cup for beam intensity measurementsA0480 55 11 ANALYSIS (CHGDS) A0480 55 12 ERR-ANALYS (DATA-ERR) The limits of error are estimated to be A0480 55 13 about 15% for most of the mass chains reported. A0480 55 14 However, at higher energies, the chain yield A0480 55 15 corrections become quite sizeable and the errors A0480 55 16 may be somewhat greater. A0480 55 17 STATUS (TABLE) Tbl. VII from Phys.Rev.,111(1958)1358 A0480 55 18 HISTORY (20200311C) SD A0480 55 19 ENDBIB 17 0 A0480 55 20 COMMON 1 3 A0480 55 21 DATA-ERR A0480 55 22 PER-CENT A0480 55 23 15. A0480 55 24 ENDCOMMON 3 0 A0480 55 25 DATA 5 72 A0480 55 26 EN ELEMENT MASS ISOMER DATA A0480 55 27 MEV NO-DIM NO-DIM NO-DIM MB A0480 55 28 22.6 40. 95. 4.7 A0480 55 29 22.6 40. 97. 8.0 A0480 55 30 22.6 44. 103. 6.5 A0480 55 31 22.6 44. 105. 7.0 A0480 55 32 22.6 48. 115. 2.6 A0480 55 33 22.6 48. 117. 1.9 A0480 55 34 22.6 56. 139. 6.5 A0480 55 35 22.6 56. 140. 5.8 A0480 55 36 25.2 58. 143. 11.5 A0480 55 37 27.1 40. 95. 29. A0480 55 38 27.1 40. 97. 36. A0480 55 39 27.1 48. 115. 15.4 A0480 55 40 27.1 58. 141. 40. A0480 55 41 27.1 58. 143. 23. A0480 55 42 27.1 60. 147. 15. A0480 55 43 27.1 63. 156. 1.8 A0480 55 44 27.1 63. 157. 1.5 A0480 55 45 27.1 65. 161. 0.29 A0480 55 46 32.5 40. 95. 21. A0480 55 47 32.5 40. 97. 34. A0480 55 48 33.8 40. 95. 28. A0480 55 49 33.8 40. 97. 41. A0480 55 50 33.8 56. 140. 29. A0480 55 51 38.6 40. 95. 38. A0480 55 52 38.6 40. 97. 54. A0480 55 53 38.6 44. 103. 47. A0480 55 54 38.6 44. 105. 36. A0480 55 55 38.6 48. 115. 48. A0480 55 56 38.6 56. 139. 36. A0480 55 57 38.6 56. 140. 35. A0480 55 58 38.6 58. 143. 44. A0480 55 59 38.6 60. 147. 27. A0480 55 60 38.6 63. 156. 3.4 A0480 55 61 38.6 63. 157. 2.5 A0480 55 62 38.6 65. 161. 0.46 A0480 55 63 40. 38. 89. 24. A0480 55 64 40. 38. 91. 27. A0480 55 65 40. 40. 95. 35. A0480 55 66 40. 40. 97. 54. A0480 55 67 40. 42. 99. 59. A0480 55 68 40. 44. 103. 44. A0480 55 69 40. 44. 105. 53. A0480 55 70 40. 46. 112. 54. A0480 55 71 40. 47. 111. 43. A0480 55 72 40. 47. 113. 49. A0480 55 73 40. 48. 115. 60. A0480 55 74 40. 52. 129. 1. 31. A0480 55 75 40. 52. 132. 39. A0480 55 76 40. 56. 140. 35. A0480 55 77 40. 58. 143. 49. A0480 55 78 40. 60. 147. 19. A0480 55 79 40. 63. 156. 4.1 A0480 55 80 40. 63. 157. 2.2 A0480 55 81 40. 64. 159. 0.71 A0480 55 82 43.9 40. 95. 41. A0480 55 83 43.9 40. 97. 53. A0480 55 84 43.9 44. 103. 51. A0480 55 85 43.9 44. 105. 55. A0480 55 86 43.9 48. 115. 58. A0480 55 87 43.9 48. 117. 61. A0480 55 88 43.9 56. 139. 37. A0480 55 89 43.9 56. 140. 36. A0480 55 90 43.9 58. 143. 30. A0480 55 91 45.4 38. 89. 27. A0480 55 92 45.4 38. 91. 35. A0480 55 93 45.4 40. 95. 36. A0480 55 94 45.4 40. 97. 52. A0480 55 95 45.4 44. 103. 47. A0480 55 96 45.4 44. 105. 48. A0480 55 97 45.4 48. 115. 49. A0480 55 98 45.4 56. 139. 42. A0480 55 99 45.4 56. 140. 36. A0480 55 100 ENDDATA 74 0 A0480 55 101 ENDSUBENT 100 0 A0480 5599999 SUBENT A0480056 20200311 A094A0480 56 1 BIB 5 15 A0480 56 2 REACTION (88-RA-226(A,4N)90-TH-226,,SIG) A0480 56 3 SAMPLE The radium used was isotopically pure Ra-226. A0480 56 4 The target material was deposited on l-mil gold plates A0480 56 5 rather than aluminum "hats" to simplify the chemical A0480 56 6 procedures following bombardment. The radium was A0480 56 7 electrodeposited on the gold foil from a solution A0480 56 8 0.15 M in sulfuric acid and 0.15 M in ammonium formate.A0480 56 9 The plating yields were rather low, but this did not A0480 56 10 present much difficulty as 0.1 mu-g was sufficient to A0480 56 11 produce adequate amounts of the 26-min. A0480 56 12 STATUS (TABLE) Tbl. VIII from UCRL-3858,1057 report. A0480 56 13 ERR-ANALYS (DATA-ERR) The estimated errors of ~ 20% are A0480 56 14 principally due to uncertainties in determining the A0480 56 15 amount of target material bombarded A0480 56 16 HISTORY (20200311C) SD A0480 56 17 ENDBIB 15 0 A0480 56 18 NOCOMMON 0 0 A0480 56 19 DATA 3 8 A0480 56 20 EN DATA DATA-ERR A0480 56 21 MEV MB MB A0480 56 22 35.6 110. 20. A0480 56 23 38.2 270. 50. A0480 56 24 39.4 260. 50. A0480 56 25 39.4 380. 80. A0480 56 26 40.8 500. 100. A0480 56 27 42.7 420. 80. A0480 56 28 44.7 490. 100. A0480 56 29 45.5 200. 40. A0480 56 30 ENDDATA 10 0 A0480 56 31 ENDSUBENT 30 0 A0480 5699999 SUBENT A0480057 20200311 A094A0480 57 1 BIB 7 15 A0480 57 2 REACTION (90-TH-230(A,4N)92-U-230,,SIG) A0480 57 3 MONITOR (94-PU-239(A,3N)96-CM-240,,SIG) The monitor reaction A0480 57 4 gave an average recoil-collection efficiency for all A0480 57 5 of the bombardment of 80 +- 5%. A0480 57 6 SAMPLE The thorium used had an isotopic composition of A0480 57 7 87.85 +- 0.1% Th-230 and 12.12 +- 0.1% Th-232. A0480 57 8 The target used for the recoil bombardments was A0480 57 9 prepared by electrodeposition of the thorium and A0480 57 10 plutonium onto a gold cathode from a 6 M ammonium A0480 57 11 chloride solution. The target was found to contain A0480 57 12 1.61 mu-g/cm2 of Th-230 and 2.43 mu-g/cm2 of Pu239. A0480 57 13 CORRECTION Corrected for recoil efficiency A0480 57 14 STATUS (TABLE) Tbl. IX from UCRL-3858,1057 report. A0480 57 15 ERR-ANALYS (DATA-ERR) No information about source of uncertainty A0480 57 16 HISTORY (20200311C) SD A0480 57 17 ENDBIB 15 0 A0480 57 18 NOCOMMON 0 0 A0480 57 19 DATA 3 6 A0480 57 20 EN DATA DATA-ERR A0480 57 21 MEV MB MB A0480 57 22 38.0 2.8 0.2 A0480 57 23 40.0 10.2 0.7 A0480 57 24 41.2 12.5 0.9 A0480 57 25 42.6 12.9 0.9 A0480 57 26 43.3 12.2 0.8 A0480 57 27 44.2 11.5 0.8 A0480 57 28 ENDDATA 8 0 A0480 57 29 ENDSUBENT 28 0 A0480 5799999 SUBENT A0480058 20200311 A094A0480 58 1 BIB 6 14 A0480 58 2 REACTION (92-U-236(A,4N)94-PU-236,,SIG) A0480 58 3 SAMPLE The uranium had an isotopic composition of 94.9% U-236,A0480 58 4 0,04% U-234, 4.52% U-235, and 0.54% U-238. The targets A0480 58 5 were electrodeposited on gold or aluminum plates by theA0480 58 6 same technique used to prepare the thorium target. A0480 58 7 The amount of material deposited was determined by A0480 58 8 direct alpha counting, and the targets usually A0480 58 9 contained about 0.1 mg of U-236 . A0480 58 10 STATUS (TABLE) Tbl. X from UCRL-3858,1057 report. A0480 58 11 COMMENT The contribution of the Pu-236 produced by the A0480 58 12 (alpha,3n) reaction from the U-235 present in the A0480 58 13 target has been subtracted. A0480 58 14 ERR-ANALYS (DATA-ERR) No information about source of uncertainty A0480 58 15 HISTORY (20200311C) SD A0480 58 16 ENDBIB 14 0 A0480 58 17 NOCOMMON 0 0 A0480 58 18 DATA 3 4 A0480 58 19 EN DATA DATA-ERR A0480 58 20 MEV MB MB A0480 58 21 34.5 9.11 0.1 A0480 58 22 38.4 2.0 0.2 A0480 58 23 42.0 4.1 0.4 A0480 58 24 45.6 3.6 0.4 A0480 58 25 ENDDATA 6 0 A0480 58 26 ENDSUBENT 25 0 A0480 5899999 ENDENTRY 58 0 A048099999999