ENTRY C2314 20180611 C176C231400000001 SUBENT C2314001 20180611 C176C231400100001 BIB 8 19 C231400100002 TITLE Helium-Ion-Induced Fission Cross Sections of U233 and C231400100003 U238 and the Nuclear Radii of Heavy Elements C231400100004 AUTHOR (L.J.Colby Jr,M.Lasalle Shoaf,J.W.Cobble) C231400100005 REFERENCE (J,PR,121,1415,1961) C231400100006 #doi:10.1103/PhysRev.121.1415 C231400100007 REL-REF (M,C2308001,R.Gunnink,J,PR,115,1247,1959) The C231400100008 particular experimental procedure and conditions for C231400100009 bombardments, chemistry, and counting. C231400100010 INSTITUTE (1USAPUR) C231400100011 FACILITY (CYCLO,1USAANL) Argonne cyclotron. C231400100012 (CYCLO,1USABRK) The Crocker cyclotron at the C231400100013 University of California. C231400100014 METHOD (CHSEP,ACTIV) A known amount (5-10 mg) of carrier C231400100015 elements in various but common oxidation states C231400100016 corresponding to each radioisotope to be used to C231400100017 determine the isobaric fission mass yield was C231400100018 combined to form a solution in which the irradiated C231400100019 target was dissolved. C231400100020 HISTORY (20180611C) BP C231400100021 ENDBIB 19 0 C231400100022 COMMON 1 3 C231400100023 EN-ERR C231400100024 MEV C231400100025 0.5 C231400100026 ENDCOMMON 3 0 C231400100027 ENDSUBENT 26 0 C231400199999 SUBENT C2314002 20180611 C176C231400200001 BIB 4 13 C231400200002 REACTION (92-U-233(A,F)ELEM/MASS,CUM,SIG) C231400200003 SAMPLE (92-U-233,ENR=1.0) The U233 was supplied by the C231400200004 University of California Radiation Laboratory. An C231400200005 alpha-spectrum analysis showed only 2.5% alpha active C231400200006 impurity in the sample. This is, therefore, C231400200007 indication of the isotopic purity y of the C231400200008 material. It was considered to be 100% U233. C231400200009 ERR-ANALYS (DATA-ERR) Experimental accuracy of the fission data. C231400200010 From the scatter of points about the smooth curves, C231400200011 it is probable that the integrated fission cross C231400200012 sections at many energies are accurate to at least C231400200013 +-10%. C231400200014 STATUS (TABLE) Table I, page 1417. C231400200015 ENDBIB 13 0 C231400200016 NOCOMMON 0 0 C231400200017 DATA 6 91 C231400200018 EN ELEMENT MASS ISOMER DATA DATA-ERR C231400200019 MEV NO-DIM NO-DIM NO-DIM MB MB C231400200020 25.3 35.0 83.0 3.4 0.1C231400200021 25.3 38.0 89.0 5.7 0.5C231400200022 25.3 38.0 91.0 10.0 0.9C231400200023 25.3 38.0 92.0 11.4 0.4C231400200024 25.3 39.0 93.0 17.0 0.4C231400200025 25.3 40.0 95.0 25.0 1.3C231400200026 25.3 40.0 97.0 21.0 1.9C231400200027 25.3 44.0 103.0 12.1 0.1C231400200028 25.3 44.0 105.0 7.6 0.1C231400200029 25.3 44.0 106.0 10.4 0.6C231400200030 25.3 46.0 112.0 7.0 C231400200031 25.3 48.0 115.0 0.0 8.0 0.5C231400200032 25.3 48.0 115.0 1.0 0.8 C231400200033 25.3 53.0 131.0 11.7 0.5C231400200034 25.3 53.0 133.0 9.0 0.5C231400200035 25.3 56.0 140.0 7.3 0.5C231400200036 25.3 58.0 141.0 12.2 1.0C231400200037 25.3 58.0 143.0 8.7 0.1C231400200038 25.3 59.0 145.0 6.0 0.1C231400200039 25.3 60.0 147.0 4.9 0.3C231400200040 25.3 62.0 153.0 1.0 0.1C231400200041 25.3 63.0 157.0 0.5 0.03C231400200042 25.3 64.0 159.0 0.2 0.02C231400200043 29.0 35.0 83.0 5.1 0.1C231400200044 29.0 38.0 89.0 11.7 0.4C231400200045 29.0 38.0 91.0 17.5 0.5C231400200046 29.0 38.0 92.0 23.5 0.9C231400200047 29.0 39.0 93.0 23.3 0.3C231400200048 29.0 40.0 95.0 34.3 0.5C231400200049 29.0 40.0 97.0 31.0 1.9C231400200050 29.0 44.0 103.0 19.2 0.3C231400200051 29.0 44.0 105.0 11.0 0.9C231400200052 29.0 44.0 106.0 15.0 0.5C231400200053 29.0 46.0 109.0 15.0 C231400200054 29.0 46.0 112.0 13.0 0.3C231400200055 29.0 47.0 113.0 16.9 C231400200056 29.0 48.0 115.0 0.0 16.0 0.9C231400200057 29.0 53.0 131.0 19.2 C231400200058 29.0 53.0 133.0 12.0 1.3C231400200059 29.0 56.0 140.0 11.4 0.4C231400200060 29.0 58.0 141.0 15.5 1.1C231400200061 29.0 58.0 143.0 13.4 0.6C231400200062 29.0 59.0 145.0 10.4 0.1C231400200063 29.0 60.0 147.0 8.9 0.2C231400200064 29.0 62.0 153.0 1.9 0.05C231400200065 29.0 63.0 157.0 0.67 C231400200066 29.0 64.0 159.0 0.27 0.05C231400200067 34.5 35.0 83.0 9.5 0.5C231400200068 34.5 38.0 89.0 21.5 0.5C231400200069 34.5 38.0 91.0 27.0 2.3C231400200070 34.5 38.0 92.0 28.5 0.5C231400200071 34.5 39.0 93.0 35.9 1.0C231400200072 34.5 40.0 95.0 46.0 0.5C231400200073 34.5 40.0 97.0 45.9 1.0C231400200074 34.5 44.0 103.0 30.0 1.0C231400200075 34.5 44.0 105.0 22.3 0.3C231400200076 34.5 44.0 106.0 31.0 0.9C231400200077 34.5 48.0 115.0 0.0 33.2 C231400200078 34.5 48.0 115.0 1.0 4.0 C231400200079 34.5 53.0 131.0 26.2 C231400200080 34.5 53.0 133.0 14.7 0.2C231400200081 34.5 56.0 140.0 11.0 C231400200082 34.5 58.0 141.0 19.3 0.7C231400200083 34.5 58.0 143.0 15.5 C231400200084 34.5 59.0 145.0 13.0 0.2C231400200085 34.5 60.0 147.0 9.0 C231400200086 34.5 62.0 153.0 2.7 0.3C231400200087 34.5 63.0 157.0 1.1 0.05C231400200088 34.5 64.0 159.0 0.55 0.05C231400200089 40.5 35.0 83.0 8.6 0.1C231400200090 40.5 38.0 89.0 22.0 1.0C231400200091 40.5 38.0 91.0 33.1 0.1C231400200092 40.5 38.0 92.0 34.8 C231400200093 40.5 39.0 93.0 38.8 0.4C231400200094 40.5 40.0 95.0 49.6 C231400200095 40.5 40.0 97.0 46.0 2.5C231400200096 40.5 44.0 103.0 44.0 2.8C231400200097 40.5 44.0 105.0 35.0 1.2C231400200098 40.5 44.0 106.0 40.0 3.2C231400200099 40.5 48.0 115.0 0.0 42.1 C231400200100 40.5 48.0 115.0 1.0 5.3 C231400200101 40.5 53.0 131.0 32.9 C231400200102 40.5 53.0 133.0 13.5 C231400200103 40.5 56.0 140.0 12.0 C231400200104 40.5 58.0 141.0 16.3 C231400200105 40.5 58.0 143.0 12.2 C231400200106 40.5 59.0 145.0 10.3 C231400200107 40.5 60.0 147.0 9.4 0.4C231400200108 40.5 62.0 153.0 2.8 0.1C231400200109 40.5 63.0 157.0 1.0 C231400200110 40.5 64.0 159.0 0.55 0.05C231400200111 ENDDATA 93 0 C231400200112 ENDSUBENT 111 0 C231400299999 SUBENT C2314003 20180611 C176C231400300001 BIB 4 13 C231400300002 REACTION (92-U-233(A,F)MASS,CHN,SIG) C231400300003 SAMPLE (92-U-233,ENR=1.0) The U233 was supplied by the C231400300004 University of California Radiation Laboratory. An C231400300005 alpha-spectrum analysis showed only 2.5% alpha active C231400300006 impurity in the sample. This is, therefore, C231400300007 indication of the isotopic purity y of the C231400300008 material. It was considered to be 100% U233. C231400300009 ANALYSIS (CHGDS) The cross sections are corrected for the value C231400300010 for that part of the mass chain which was not directly C231400300011 determined using the correlations based on the C231400300012 constant-charge-ratio (C.C.R.) rule. C231400300013 STATUS (TABLE) Table I, page 1417. C231400300014 (DEP,C2315002) Cumulative cross section C231400300015 ENDBIB 13 0 C231400300016 NOCOMMON 0 0 C231400300017 DATA 3 88 C231400300018 EN MASS DATA C231400300019 MEV NO-DIM MB C231400300020 25.3 83.0 3.5 C231400300021 25.3 89.0 5.7 C231400300022 25.3 91.0 10.2 C231400300023 25.3 92.0 12.1 C231400300024 25.3 93.0 17.3 C231400300025 25.3 95.0 25.0 C231400300026 25.3 97.0 22.4 C231400300027 25.3 103.0 12.1 C231400300028 25.3 105.0 9.3 C231400300029 25.3 106.0 10.8 C231400300030 25.3 112.0 7.5 C231400300031 25.3 115.0 8.9 C231400300032 25.3 131.0 15.6 C231400300033 25.3 133.0 21.0 C231400300034 25.3 140.0 14.0 C231400300035 25.3 141.0 13.1 C231400300036 25.3 143.0 10.4 C231400300037 25.3 145.0 6.8 C231400300038 25.3 147.0 5.3 C231400300039 25.3 153.0 1.2 C231400300040 25.3 157.0 0.8 C231400300041 25.3 159.0 0.3 C231400300042 29.0 83.0 5.2 C231400300043 29.0 89.0 11.7 C231400300044 29.0 91.0 18.1 C231400300045 29.0 92.0 25.3 C231400300046 29.0 93.0 23.8 C231400300047 29.0 95.0 34.6 C231400300048 29.0 97.0 33.2 C231400300049 29.0 103.0 19.2 C231400300050 29.0 105.0 13.4 C231400300051 29.0 106.0 15.6 C231400300052 29.0 109.0 15.0 C231400300053 29.0 112.0 14.1 C231400300054 29.0 113.0 17.2 C231400300055 29.0 115.0 18.0 C231400300056 29.0 131.0 29.3 C231400300057 29.0 133.0 31.0 C231400300058 29.0 140.0 26.0 C231400300059 29.0 141.0 22.0 C231400300060 29.0 143.0 16.5 C231400300061 29.0 145.0 12.1 C231400300062 29.0 147.0 10.0 C231400300063 29.0 153.0 2.4 C231400300064 29.0 157.0 1.26 C231400300065 29.0 159.0 0.44 C231400300066 34.5 83.0 9.5 C231400300067 34.5 89.0 21.5 C231400300068 34.5 91.0 27.8 C231400300069 34.5 92.0 31.0 C231400300070 34.5 93.0 36.6 C231400300071 34.5 95.0 46.4 C231400300072 34.5 97.0 48.5 C231400300073 34.5 103.0 30.0 C231400300074 34.5 105.0 27.1 C231400300075 34.5 106.0 32.3 C231400300076 34.5 115.0 37.5 C231400300077 34.5 131.0 36.4 C231400300078 34.5 133.0 44.5 C231400300079 34.5 140.0 28.2 C231400300080 34.5 141.0 25.6 C231400300081 34.5 143.0 20.2 C231400300082 34.5 145.0 15.7 C231400300083 34.5 147.0 10.3 C231400300084 34.5 153.0 3.6 C231400300085 34.5 157.0 2.4 C231400300086 34.5 159.0 1.0 C231400300087 40.5 83.0 8.7 C231400300088 40.5 89.0 22.2 C231400300089 40.5 91.0 34.4 C231400300090 40.5 92.0 39.2 C231400300091 40.5 93.0 40.0 C231400300092 40.5 95.0 50.6 C231400300093 40.5 97.0 51.7 C231400300094 40.5 103.0 44.0 C231400300095 40.5 105.0 43.1 C231400300096 40.5 106.0 42.5 C231400300097 40.5 115.0 48.5 C231400300098 40.5 131.0 51.0 C231400300099 40.5 133.0 56.0 C231400300100 40.5 140.0 42.8 C231400300101 40.5 141.0 33.4 C231400300102 40.5 143.0 18.8 C231400300103 40.5 145.0 13.9 C231400300104 40.5 147.0 11.4 C231400300105 40.5 153.0 4.4 C231400300106 40.5 157.0 3.1 C231400300107 40.5 159.0 1.3 C231400300108 ENDDATA 90 0 C231400300109 ENDSUBENT 108 0 C231400399999 SUBENT C2314004 20180611 C176C231400400001 BIB 4 9 C231400400002 REACTION (92-U-238(A,F)ELEM/MASS,CUM,SIG) C231400400003 SAMPLE (92-U-238,ENR=1.0) Natural uranium was used for the C231400400004 U238 bombardments and considered to be 100% U238. C231400400005 ERR-ANALYS (DATA-ERR) Experimental accuracy of the fission data. C231400400006 From the scatter of points about the smooth curves, C231400400007 it is probable that the integrated 6ssion cross C231400400008 sections at many energies are accurate to at least C231400400009 +-10%. C231400400010 STATUS (TABLE) Table II, page 1419. C231400400011 ENDBIB 9 0 C231400400012 NOCOMMON 0 0 C231400400013 DATA 5 104 C231400400014 EN ELEMENT MASS DATA DATA-ERR C231400400015 MEV NO-DIM NO-DIM MB MB C231400400016 19.8 38.0 91.0 0.24 C231400400017 19.8 40.0 95.0 0.53 C231400400018 19.8 40.0 97.0 0.63 C231400400019 19.8 44.0 103.0 0.40 C231400400020 19.8 46.0 112.0 0.057 C231400400021 19.8 48.0 115.0 0.099 C231400400022 19.8 53.0 131.0 0.276 C231400400023 19.8 53.0 133.0 0.388 C231400400024 19.8 56.0 140.0 0.641 C231400400025 19.8 58.0 141.0 0.67 C231400400026 19.8 58.0 143.0 0.50 C231400400027 19.8 60.0 147.0 0.166 C231400400028 19.8 62.0 153.0 0.028 C231400400029 24.1 38.0 91.0 1.1 0.1 C231400400030 24.1 39.0 93.0 3.5 C231400400031 24.1 40.0 95.0 5.8 0.1 C231400400032 24.1 40.0 97.0 6.6 C231400400033 24.1 44.0 103.0 5.48 C231400400034 24.1 44.0 105.0 4.74 C231400400035 24.1 46.0 112.0 2.0 0.1 C231400400036 24.1 48.0 115.0 1.48 C231400400037 24.1 53.0 131.0 3.71 0.4 C231400400038 24.1 53.0 133.0 4.1 0.1 C231400400039 24.1 56.0 140.0 5.7 0.1 C231400400040 24.1 58.0 141.0 5.1 C231400400041 24.1 58.0 143.0 5.2 C231400400042 24.1 60.0 147.0 2.43 0.15 C231400400043 24.1 62.0 153.0 0.68 C231400400044 31.0 38.0 89.0 3.6 C231400400045 31.0 38.0 91.0 15.6 C231400400046 31.0 39.0 93.0 22.0 0.2 C231400400047 31.0 40.0 95.0 35.1 1.5 C231400400048 31.0 40.0 97.0 37.2 1.3 C231400400049 31.0 44.0 105.0 27.7 C231400400050 31.0 46.0 112.0 19.0 0.5 C231400400051 31.0 48.0 115.0 16.3 C231400400052 31.0 53.0 131.0 25.4 C231400400053 31.0 53.0 133.0 26.3 1.7 C231400400054 31.0 56.0 140.0 30.8 0.9 C231400400055 31.0 58.0 141.0 29.2 C231400400056 31.0 58.0 143.0 27.3 0.1 C231400400057 31.0 60.0 147.0 6.74 0.1 C231400400058 31.0 62.0 153.0 0.40 C231400400059 33.8 35.0 83.0 2.7 0.3 C231400400060 33.8 38.0 89.0 8.8 0.9 C231400400061 33.8 38.0 91.0 16.5 0.7 C231400400062 33.8 38.0 92.0 17.7 1.1 C231400400063 33.8 39.0 93.0 29.7 1.6 C231400400064 33.8 40.0 95.0 43.5 2.8 C231400400065 33.8 40.0 97.0 42.8 1.9 C231400400066 33.8 44.0 103.0 42.0 0.7 C231400400067 33.8 44.0 105.0 31.8 1.3 C231400400068 33.8 44.0 106.0 36.4 0.4 C231400400069 33.8 48.0 115.0 22.0 C231400400070 33.8 53.0 131.0 29.1 0.6 C231400400071 33.8 53.0 133.0 31.4 0.5 C231400400072 33.8 58.0 141.0 33.4 33.4 C231400400073 33.8 58.0 143.0 27.8 28.4 C231400400074 33.8 59.0 145.0 17.9 1.9 C231400400075 33.8 60.0 147.0 13.0 1.0 C231400400076 33.8 62.0 153.0 3.5 0.5 C231400400077 33.8 63.0 157.0 1.6 0.5 C231400400078 33.8 64.0 159.0 1.0 0.3 C231400400079 36.8 35.0 83.0 2.2 C231400400080 36.8 38.0 89.0 22.5 C231400400081 36.8 38.0 91.0 29.4 0.9 C231400400082 36.8 39.0 93.0 35.6 1.4 C231400400083 36.8 40.0 95.0 48.6 2.6 C231400400084 36.8 40.0 97.0 47.2 0.4 C231400400085 36.8 44.0 103.0 43.8 C231400400086 36.8 44.0 105.0 37.5 C231400400087 36.8 46.0 112.0 30.4 2.1 C231400400088 36.8 48.0 115.0 30.4 C231400400089 36.8 53.0 131.0 31.6 1.6 C231400400090 36.8 56.0 140.0 31.1 0.6 C231400400091 36.8 58.0 141.0 27.2 1.7 C231400400092 36.8 58.0 143.0 28.2 0.4 C231400400093 36.8 60.0 147.0 15.1 0.4 C231400400094 36.8 62.0 153.0 2.1 0.2 C231400400095 36.8 64.0 159.0 1.0 C231400400096 39.9 30.0 72.0 0.54 C231400400097 39.9 35.0 83.0 5.3 0.5 C231400400098 39.9 38.0 89.0 14.0 1.0 C231400400099 39.9 38.0 91.0 29.0 2.0 C231400400100 39.9 38.0 92.0 32.1 1.0 C231400400101 39.9 39.0 93.0 40.4 1.3 C231400400102 39.9 40.0 95.0 50.5 1.8 C231400400103 39.9 40.0 97.0 49.6 2.4 C231400400104 39.9 44.0 103.0 49.7 3.0 C231400400105 39.9 44.0 105.0 37.6 1.3 C231400400106 39.9 44.0 106.0 42.3 0.3 C231400400107 39.9 46.0 112.0 39.6 C231400400108 39.9 48.0 115.0 37.3 0.8 C231400400109 39.9 53.0 131.0 40.9 1.1 C231400400110 39.9 53.0 133.0 39.4 C231400400111 39.9 56.0 139.0 43.9 C231400400112 39.9 56.0 140.0 37.5 2.5 C231400400113 39.9 58.0 141.0 47.2 0.3 C231400400114 39.9 58.0 143.0 43.0 0.5 C231400400115 39.9 59.0 145.0 35.7 0.6 C231400400116 39.9 60.0 147.0 19.0 0.9 C231400400117 39.9 62.0 153.0 5.5 0.8 C231400400118 39.9 63.0 157.0 1.8 0.2 C231400400119 39.9 64.0 159.0 1.5 0.1 C231400400120 ENDDATA 106 0 C231400400121 ENDSUBENT 120 0 C231400499999 SUBENT C2314005 20180611 C176C231400500001 BIB 4 9 C231400500002 REACTION (92-U-238(A,F)MASS,CHN,SIG) C231400500003 SAMPLE (92-U-238,ENR=1.0) Natural uranium was used for the C231400500004 U238 bombardments and considered to be 100% U238. C231400500005 ANALYSIS (CHGDS) The cross sections are corrected for the value C231400500006 for that part of the mass chain which was not directly C231400500007 determined using the correlations based on the C231400500008 constant-charge-ratio (C.C.R.) rule. C231400500009 STATUS (TABLE) Table II, page 1419. C231400500010 (DEP,C2315004) Cumulative cross section C231400500011 ENDBIB 9 0 C231400500012 NOCOMMON 0 0 C231400500013 DATA 3 89 C231400500014 EN MASS DATA C231400500015 MEV NO-DIM MB C231400500016 24.1 91.0 1.1 C231400500017 24.1 93.0 3.5 C231400500018 24.1 95.0 5.8 C231400500019 24.1 97.0 6.6 C231400500020 24.1 103.0 5.48 C231400500021 24.1 105.0 4.74 C231400500022 24.1 112.0 2.0 C231400500023 24.1 115.0 1.48 C231400500024 24.1 131.0 3.79 C231400500025 24.1 133.0 4.71 C231400500026 24.1 140.0 6.2 C231400500027 24.1 141.0 5.1 C231400500028 24.1 143.0 5.2 C231400500029 24.1 147.0 2.43 C231400500030 24.1 153.0 0.68 C231400500031 31.0 89.0 3.6 C231400500032 31.0 91.0 15.6 C231400500033 31.0 93.0 22.0 C231400500034 31.0 95.0 35.1 C231400500035 31.0 97.0 37.5 C231400500036 31.0 105.0 27.7 C231400500037 31.0 112.0 19.2 C231400500038 31.0 115.0 16.3 C231400500039 31.0 131.0 26.4 C231400500040 31.0 133.0 31.7 C231400500041 31.0 140.0 35.0 C231400500042 31.0 141.0 29.2 C231400500043 31.0 143.0 27.9 C231400500044 31.0 147.0 6.80 C231400500045 31.0 153.0 0.41 C231400500046 33.8 83.0 2.78 C231400500047 33.8 89.0 8.8 C231400500048 33.8 91.0 16.5 C231400500049 33.8 92.0 17.8 C231400500050 33.8 93.0 29.8 C231400500051 33.8 95.0 43.5 C231400500052 33.8 97.0 43.2 C231400500053 33.8 103.0 42.0 C231400500054 33.8 105.0 38.4 C231400500055 33.8 106.0 36.6 C231400500056 33.8 115.0 22.0 C231400500057 33.8 131.0 30.3 C231400500058 33.8 133.0 37.8 C231400500059 33.8 145.0 18.3 C231400500060 33.8 147.0 13.1 C231400500061 33.8 153.0 3.57 C231400500062 33.8 157.0 1.75 C231400500063 33.8 159.0 1.04 C231400500064 36.8 83.0 2.27 C231400500065 36.8 89.0 22.5 C231400500066 36.8 91.0 29.5 C231400500067 36.8 93.0 35.9 C231400500068 36.8 95.0 48.6 C231400500069 36.8 97.0 47.6 C231400500070 36.8 103.0 43.8 C231400500071 36.8 105.0 37.5 C231400500072 36.8 112.0 31.0 C231400500073 36.8 115.0 30.4 C231400500074 36.8 131.0 33.3 C231400500075 36.8 140.0 36.6 C231400500076 36.8 141.0 27.5 C231400500077 36.8 143.0 29.0 C231400500078 36.8 147.0 15.3 C231400500079 36.8 153.0 2.14 C231400500080 36.8 159.0 1.06 C231400500081 39.9 72.0 0.54 C231400500082 39.9 83.0 5.52 C231400500083 39.9 89.0 14.0 C231400500084 39.9 91.0 29.3 C231400500085 39.9 92.0 32.7 C231400500086 39.9 93.0 40.8 C231400500087 39.9 95.0 51.0 C231400500088 39.9 97.0 50.6 C231400500089 39.9 103.0 49.7 C231400500090 39.9 105.0 46.0 C231400500091 39.9 106.0 43.1 C231400500092 39.9 112.0 39.6 C231400500093 39.9 115.0 37.3 C231400500094 39.9 131.0 43.5 C231400500095 39.9 133.0 53.2 C231400500096 39.9 139.0 48.2 C231400500097 39.9 140.0 46.3 C231400500098 39.9 141.0 47.2 C231400500099 39.9 143.0 44.8 C231400500100 39.9 145.0 36.8 C231400500101 39.9 147.0 19.4 C231400500102 39.9 153.0 5.73 C231400500103 39.9 157.0 2.09 C231400500104 39.9 159.0 1.63 C231400500105 ENDDATA 91 0 C231400500106 ENDSUBENT 105 0 C231400599999 SUBENT C2314006 20180611 C176C231400600001 BIB 3 10 C231400600002 REACTION (92-U-233(A,F),,SIG,,,DERIV) C231400600003 SAMPLE (92-U-233,ENR=1.0) The U233 was supplied by the C231400600004 University of California Radiation Laboratory. An C231400600005 alpha-spectrum analysis showed only 2.5% alpha active C231400600006 impurity in the sample. This is, therefore, C231400600007 indication of the isotopic purity of the C231400600008 material. It was considered to be 100% U233. C231400600009 STATUS (DEP,C2314002) C231400600010 (DEP,C2314003) C231400600011 (TABLE) Table III, page 1419. C231400600012 ENDBIB 10 0 C231400600013 NOCOMMON 0 0 C231400600014 DATA 2 4 C231400600015 EN DATA C231400600016 MEV MB C231400600017 25.3 350.0 C231400600018 29.0 606.0 C231400600019 34.5 1090.0 C231400600020 40.5 1345.0 C231400600021 ENDDATA 6 0 C231400600022 ENDSUBENT 21 0 C231400699999 SUBENT C2314007 20180611 C176C231400700001 BIB 3 6 C231400700002 REACTION (92-U-238(A,F),,SIG,,,DERIV) C231400700003 SAMPLE (92-U-238,ENR=1.0) Natural uranium was used for the C231400700004 U238 bombardments and considered to be 100% U238. C231400700005 STATUS (DEP,C2314004) C231400700006 (DEP,C2314005) C231400700007 (TABLE) Table III, page 1419. C231400700008 ENDBIB 6 0 C231400700009 NOCOMMON 0 0 C231400700010 DATA 2 6 C231400700011 EN DATA C231400700012 MEV MB C231400700013 19.8 5.4 C231400700014 24.2 168.0 C231400700015 31.0 800.0 C231400700016 33.8 970.0 C231400700017 36.8 1127.0 C231400700018 39.9 1317.0 C231400700019 ENDDATA 8 0 C231400700020 ENDSUBENT 19 0 C231400799999 ENDENTRY 7 0 C231499999999