ENTRY 13073 20180302 14391307300000001 SUBENT 13073001 20180302 14391307300100001 BIB 8 21 1307300100002 TITLE Nuclear-Charge Distribution of Fission-Product Chains 1307300100003 of Mass Numbers 131-133 1307300100004 AUTHOR (P.O.Strom,D.L.Love,A.E.Greendale,A.A.Delucchi,D.Sam, 1307300100005 N.E.Ballou) 1307300100006 REFERENCE (J,PR,144,984,196604) 1307300100007 #doi:10.1103/PhysRev.144.984 1307300100008 REL-REF (M,14304001,A.E.Greendale+,J,AC,35,(11),1712,1963) 1307300100009 Chemical separation procedures, early results on tin. 1307300100010 INSTITUTE (1USANRD) 1307300100011 FACILITY (REAC,1USASTF) The 10-kW reactor of the Nuclear 1307300100012 Technology Laboratory of Stanford University. 1307300100013 INC-SPECT Reactor spectrum: The neutron flux in the area of 1307300100014 bombardment was approximately 10**10 n/cm2-sec and 1307300100015 the cadmium ratio for gold was determined to be 12+-2 1307300100016 under the conditions of the experiments. 1307300100017 HISTORY (19890606C) VM 1307300100018 (20021204A) Converted to new date formats, lower case. 1307300100019 BIB updated. 1307300100020 (20180302A) BP: Added the Table III data: chain and 1307300100021 fractional yields, updated the entry, 1307300100022 added doi. 1307300100023 ENDBIB 21 0 1307300100024 COMMON 1 3 1307300100025 EN-DUMMY 1307300100026 EV 1307300100027 0.0253 1307300100028 ENDCOMMON 3 0 1307300100029 ENDSUBENT 28 0 1307300199999 SUBENT 13073002 20180302 14391307300200001 BIB 7 17 1307300200002 REACTION (92-U-235(N,F)ELEM/MASS,CUM,FY,,SPA) 1307300200003 METHOD (CHSEP) 1307300200004 MONITOR (79-AU-197(N,G)79-AU-198,,SIG) Flux monitor 1307300200005 ((MONIT1)92-U-235(N,F)42-MO-99,CUM,FY,,SPA) 1307300200006 ((MONIT2)92-U-235(N,F)56-BA-139,CUM,FY,,SPA) 1307300200007 ((MONIT3)92-U-235(N,F)56-BA-140,CUM,FY,,SPA) 1307300200008 MONIT-REF ((MONIT1)13064001,H.Farrar+,J,NP,34,367,1962) 1307300200009 ((MONIT2)13064001,H.Farrar+,J,NP,34,367,1962) 1307300200010 ((MONIT3)13064001,H.Farrar+,J,NP,34,367,1962) 1307300200011 ERR-ANALYS (DATA-ERR) Data uncertainty given is probably 1307300200012 standard deviation. It is reported as a standard error.1307300200013 DECAY-DATA ((1.)50-SN-131-G,1.32MIN) 1307300200014 ((2.)50-SN-132,1.00MIN) 1307300200015 ((3.)50-SN-133,55.SEC) 1307300200016 ((4.)51-SB-133,2.67MIN) 1307300200017 *** Comment by compiler: Half lives are out of date. 1307300200018 STATUS (TABLE) Table II, page 988. 1307300200019 ENDBIB 17 0 1307300200020 COMMON 3 3 1307300200021 MONIT1 MONIT2 MONIT3 1307300200022 PC/FIS PC/FIS PC/FIS 1307300200023 6.25 6.42 6.25 1307300200024 ENDCOMMON 3 0 1307300200025 DATA 7 4 1307300200026 ELEMENT MASS ISOMER DATA DATA-ERR DATA-MAX 1307300200027 DECAY-FLAG 1307300200028 NO-DIM NO-DIM NO-DIM PC/FIS PC/FIS PC/FIS 1307300200029 NO-DIM 1307300200030 50. 131. 0. 1.28 0.21 1307300200031 1. 1307300200032 50. 132. 0.59 0.04 1307300200033 2. 1307300200034 50. 133. 0.0151307300200035 3. 1307300200036 51. 133. 3.05 0.39 1307300200037 4. 1307300200038 ENDDATA 12 0 1307300200039 ENDSUBENT 38 0 1307300299999 SUBENT 13073003 20180302 14391307300300001 BIB 8 21 1307300300002 REACTION (92-U-235(N,F)ELEM/MASS,IND,FY,,SPA) 1307300300003 METHOD (CHSEP) 1307300300004 MONITOR (79-AU-197(N,G)79-AU-198,,SIG) Flux monitor 1307300300005 ((MONIT1)92-U-235(N,F)42-MO-99,CUM,FY,,SPA) 1307300300006 ((MONIT2)92-U-235(N,F)56-BA-139,CUM,FY,,SPA) 1307300300007 ((MONIT3)92-U-235(N,F)56-BA-140,CUM,FY,,SPA) 1307300300008 MONIT-REF ((MONIT1)13064001,H.Farrar+,J,NP,34,367,1962) 1307300300009 ((MONIT2)13064001,H.Farrar+,J,NP,34,367,1962) 1307300300010 ((MONIT3)13064001,H.Farrar+,J,NP,34,367,1962) 1307300300011 ERR-ANALYS (DATA-ERR) Data uncertainty given is probably 1307300300012 standard deviation. It is reported as a standard error.1307300300013 DECAY-DATA ((1.)51-SB-131,23.MIN) 1307300300014 ((2.)51-SB-132-M,3.13MIN) 1307300300015 *** Comment by compiler: Half life out of date. 1307300300016 ((4.)52-TE-132,77.HR) 1307300300017 *** Comment by compiler: Half life out of date. 1307300300018 ((5.)52-TE-133-G,12.45MIN) 1307300300019 ((6.)52-TE-133-M,50.MIN) 1307300300020 ((7.)53-I-133-G,20.8HR) 1307300300021 STATUS (TABLE) Table II, page 988. 1307300300022 HISTORY (20021204A) Flags updated. 1307300300023 ENDBIB 21 0 1307300300024 COMMON 3 3 1307300300025 MONIT1 MONIT2 MONIT3 1307300300026 PC/FIS PC/FIS PC/FIS 1307300300027 6.25 6.42 6.25 1307300300028 ENDCOMMON 3 0 1307300300029 DATA 6 6 1307300300030 ELEMENT MASS ISOMER DATA DATA-ERR DECAY-FLAG 1307300300031 NO-DIM NO-DIM NO-DIM PC/FIS PC/FIS NO-DIM 1307300300032 51. 131. 1.66 0.40 1.1307300300033 51. 132. 1. 2.76 0.35 2.1307300300034 52. 132. 0.86 0.10 4.1307300300035 52. 133. 0. 2.07 0.31 5.1307300300036 52. 133. 1. 2.19 0.33 6.1307300300037 53. 133. 0.17 0.06 7.1307300300038 ENDDATA 8 0 1307300300039 ENDSUBENT 38 0 1307300399999 SUBENT 13073004 20180302 14391307300400001 BIB 7 15 1307300400002 REACTION (92-U-235(N,F)MASS,CHN,FY,,SPA) 1307300400003 REL-REF (E,13080001,D.G.Sarantites+,J,PR,138,B353,1965) 1307300400004 (E,,S.Katcoff,J,NUC,18,201,1960) These references 1307300400005 were used to derive 52-Te-131-G and 52-Te-131-M 1307300400006 contributions. 1307300400007 METHOD The total yield of each mass chain, obtained by 1307300400008 taking the sum of indidual yields. 1307300400009 ERR-ANALYS (DATA-ERR) No details on sources of uncertainties. 1307300400010 FLAG (1.) 52-Te-131 yields were derived from Sarantites 1307300400011 fractional independent yield and the total chain 1307300400012 yield as given by Katcoff. 1307300400013 STATUS (DEP,13073002) 1307300400014 (DEP,13073003) 1307300400015 (TABLE) Table III, page 992. 1307300400016 HISTORY (20180302C) BP 1307300400017 ENDBIB 15 0 1307300400018 NOCOMMON 0 0 1307300400019 DATA 4 3 1307300400020 MASS DATA DATA-ERR FLAG 1307300400021 NO-DIM PC/FIS PC/FIS NO-DIM 1307300400022 131.0 3.30 0.45 1. 1307300400023 132.0 4.21 0.40 1307300400024 133.0 7.48 0.60 1307300400025 ENDDATA 5 0 1307300400026 ENDSUBENT 25 0 1307300499999 SUBENT 13073005 20180302 14391307300500001 BIB 5 9 1307300500002 REACTION ((92-U-235(N,F)ELEM/MASS,IND,FY,,SPA)/ 1307300500003 (92-U-235(N,F)MASS,CHN,FY,,SPA)) 1307300500004 ERR-ANALYS (DATA-ERR) No details on sources of uncertainties. 1307300500005 RESULT (FRIND) 1307300500006 STATUS (DEP,13073002) 1307300500007 (DEP,13073003) 1307300500008 (DEP,13073004) 1307300500009 (TABLE) Table III, page 992. 1307300500010 HISTORY (20180302C) BP 1307300500011 ENDBIB 9 0 1307300500012 NOCOMMON 0 0 1307300500013 DATA 4 8 1307300500014 MASS ELEMENT DATA DATA-ERR 1307300500015 NO-DIM NO-DIM NO-DIM NO-DIM 1307300500016 131.0 50.0 0.39 0.08 1307300500017 131.0 51.0 0.50 0.14 1307300500018 132.0 50.0 0.14 0.04 1307300500019 132.0 51.0 0.66 0.10 1307300500020 132.0 52.0 0.20 0.03 1307300500021 133.0 51.0 0.41 0.06 1307300500022 133.0 52.0 0.57 0.13 1307300500023 133.0 53.0 0.023 0.008 1307300500024 ENDDATA 10 0 1307300500025 ENDSUBENT 24 0 1307300599999 SUBENT 13073006 20180302 14391307300600001 BIB 5 11 1307300600002 REACTION (92-U-235(N,F)MASS,,ZP,,SPA) 1307300600003 ANALYSIS The equations of best fit for each mass chain are 1307300600004 given as P(Z)=A exp(-(Z-Zp)**2/c), where P(Z) is the 1307300600005 fractional independent yield of the radionuclide with 1307300600006 charge Z, A is the maximum value of the function, Zp 1307300600007 is the most probable charge (mean of distribution), 1307300600008 and c is the measure of the width of the distribution. 1307300600009 ERR-ANALYS (DATA-ERR) No details on sources of uncertainties. 1307300600010 STATUS (DEP,13073005) 1307300600011 (TABLE) Table III, page 992. 1307300600012 HISTORY (20180302C) BP 1307300600013 ENDBIB 11 0 1307300600014 NOCOMMON 0 0 1307300600015 DATA 3 3 1307300600016 MASS DATA DATA-ERR 1307300600017 NO-DIM NO-DIM NO-DIM 1307300600018 131.0 50.72 0.07 1307300600019 132.0 51.07 0.06 1307300600020 133.0 51.59 0.04 1307300600021 ENDDATA 5 0 1307300600022 ENDSUBENT 21 0 1307300699999 ENDENTRY 6 0 1307399999999