ENTRY 21567 20160725 22522156700000001 SUBENT 21567001 20160725 22522156700100001 BIB 13 46 2156700100002 INSTITUTE (2FR GRE) 2156700100003 REFERENCE (T,FEU ALVIM,19750612) FRNC-TH-584. 2156700100004 (J,JPR,38,273,197703) 2156700100005 (J,CEC,29,(7),347,197706) abstract 2156700100006 (R,CEA-N-1817,1,1975) Kr,Xe yields. 2156700100007 AUTHOR (C.Feu Alvim) 2156700100008 TITLE Measurement of the mass and charge distributions 2156700100009 in neutron induced fission at medium energy by 2156700100010 an emanation method (In French) 2156700100011 FACILITY (VDG,2FR GRE) 300 keV deuteron accelerator S.A.M.E.S. 2156700100012 INC-SOURCE (D-T) Deuteron-tritium reaction. 300 keV 2156700100013 deuterons onto tritiated target of 30 mm diam. 2156700100014 SAMPLE Uranylstearate or thorium stearate. Emanation 2156700100015 tests were done on each sample. 2156700100016 METHOD (CHSEP) Chemical separation. Rare gases are 2156700100017 extracted from the fission target by pumping 2156700100018 in vacuum after or during irradiation. In 2156700100019 some cases the irradiated material was passed 2156700100020 over a resin as to reduce Compton background 2156700100021 and peak interferences in their gamma-counting. 2156700100022 Using the formulas - 2156700100023 F = (Y-cum(elem) - Y-cum(rare gas))/ 2156700100024 (Y-cum(elem) and 2156700100025 F = n1*n4/(n2*n3) where 2156700100026 n1= counting rate during irradiation, 2156700100027 n2= counting rate after irradiation, 2156700100028 n3= counting rate during irradiation for 2156700100029 a reference material. 2156700100030 N4= counting rate after irradiation for 2156700100031 a reference material. 2156700100032 Fractional yields can be derived. 2156700100033 DETECTOR (GELI) Coaxial Ge(Li)-detector, 43 cc, FWNM-resol at 2156700100034 the 1332 keV-line of Co-60 is 2.35 keV, peak/Compton 2156700100035 ratio 26., efficiency with respect to a Na-I 2156700100036 of 76*76 mm*mm at 25 cm from source is 7.% 2156700100037 (GELI ) 52 cc Ge(Li) detector, resolution less than 2156700100038 2.1 keV, p/c ratio better than 32. 2156700100039 COMMENT Decay data from private comm., J.Blachot and C.Chauvin2156700100040 Two other experimental methods are described. 2156700100041 ERR-ANALYS (DATA-ERR) Quadratic error propagation used in the 2156700100042 formula F=n1*n4/(n2*n3). 2156700100043 STATUS (TABLE) Text, thesis. 2156700100044 HISTORY (19800606C) G.C. 2156700100045 (20160725A) SD:Updated to new date formats,lower case. 2156700100046 Ref. corrected (extra comma deleted). BIB corrections 2156700100047 were made following JPR,38,273,1977. Thesis unreachable2156700100048 ENDBIB 46 0 2156700100049 COMMON 2 3 2156700100050 EN EN-RSL 2156700100051 MEV MEV 2156700100052 14.7 0.5 2156700100053 ENDCOMMON 3 0 2156700100054 ENDSUBENT 53 0 2156700199999 SUBENT 21567002 20160725 22522156700200001 BIB 4 6 2156700200002 REACTION ((92-U-238(N,F)ELEM/MASS,CUM,FY)/ 2156700200003 (92-U-238(N,F)MASS,CHN,FY)) 2156700200004 RESULT (FRCUM) Fractional cumulative yields. 2156700200005 STATUS (TABLE) Table 8-1, p.64, Thesis. The same data 2156700200006 presented in Tbl. I of JPR,38,273,1977 2156700200007 HISTORY (20160725U) SD: RESULT was added. 2156700200008 ENDBIB 6 0 2156700200009 NOCOMMON 0 0 2156700200010 DATA 4 10 2156700200011 ELEMENT MASS DATA DATA-ERR 2156700200012 NO-DIM NO-DIM NO-DIM NO-DIM 2156700200013 36. 89. 0.97 0.01 2156700200014 36. 91. 0.643 0.007 2156700200015 36. 92. 0.444 0.006 2156700200016 36. 93. 0.158 0.020 2156700200017 36. 95. 0.015 0.020 2156700200018 54. 138. 0.842 0.002 2156700200019 54. 139. 0.709 0.007 2156700200020 54. 140. 0.616 0.005 2156700200021 54. 141. 0.305 0.014 2156700200022 54. 142. 0.112 0.011 2156700200023 ENDDATA 12 0 2156700200024 ENDSUBENT 23 0 2156700299999 SUBENT 21567003 20160725 22522156700300001 BIB 4 6 2156700300002 REACTION ((90-TH-232(N,F)ELEM/MASS,CUM,FY)/ 2156700300003 (90-TH-232(N,F)MASS,CHN,FY)) 2156700300004 RESULT (FRCUM) Fractional cumulative yields. 2156700300005 STATUS (TABLE) Table 8-2, p.65, Thesis. The same data 2156700300006 presented in Tbl. II of JPR,38,273,1977 2156700300007 HISTORY (20160725U) SD: RESULT was added. 2156700300008 ENDBIB 6 0 2156700300009 NOCOMMON 0 0 2156700300010 DATA 4 10 2156700300011 ELEMENT MASS DATA DATA-ERR 2156700300012 NO-DIM NO-DIM NO-DIM NO-DIM 2156700300013 36. 89. 0.955 0.02 2156700300014 36. 91. 0.62 0.02 2156700300015 36. 92. 0.38 0.02 2156700300016 36. 93. 0.20 0.03 2156700300017 36. 94. 0.07 0.07 2156700300018 54. 138. 0.909 0.009 2156700300019 54. 139. 0.815 0.010 2156700300020 54. 140. 0.61 0.07 2156700300021 54. 141. 0.28 0.05 2156700300022 54. 142. 0.10 0.02 2156700300023 ENDDATA 12 0 2156700300024 ENDSUBENT 23 0 2156700399999 SUBENT 21567004 20160725 22522156700400001 BIB 2 3 2156700400002 REACTION (92-U-238(N,F)MASS,,ZP) Most probable charge. 2156700400003 STATUS (TABLE) Table, p.92, Thesis. Similar data 2156700400004 presented in Tbl. VI of JPR,38,273,1977 2156700400005 ENDBIB 3 0 2156700400006 NOCOMMON 0 0 2156700400007 DATA 3 13 2156700400008 MASS DATA DATA-ERR 2156700400009 NO-DIM NO-DIM NO-DIM 2156700400010 87. 34.50 0.08 2156700400011 88. 35.09 0.04 2156700400012 89. 35.48 0.06 2156700400013 90. 35.91 0.06 2156700400014 91. 36.29 0.11 2156700400015 92. 36.66 0.03 2156700400016 93. 37.09 0.05 2156700400017 137. 53.50 0.07 2156700400018 138. 53.78 0.03 2156700400019 139. 54.07 0.04 2156700400020 140. 54.35 0.03 2156700400021 141. 54.76 0.03 2156700400022 142. 55.17 0.04 2156700400023 ENDDATA 15 0 2156700400024 ENDSUBENT 23 0 2156700499999 SUBENT 21567005 20160725 22522156700500001 BIB 2 4 2156700500002 REACTION (90-TH-232(N,F)MASS,,ZP) Most probable charge 2156700500003 for a given mass. 2156700500004 STATUS (TABLE) Table, p.93, Thesis. Similar data 2156700500005 presented in Tbl. VI of JPR,38,273,1977 2156700500006 ENDBIB 4 0 2156700500007 NOCOMMON 0 0 2156700500008 DATA 3 13 2156700500009 MASS DATA DATA-ERR 2156700500010 NO-DIM NO-DIM NO-DIM 2156700500011 87. 34.71 0.05 2156700500012 88. 35.22 0.04 2156700500013 89. 35.47 0.05 2156700500014 90. 35.99 0.03 2156700500015 91. 36.37 0.04 2156700500016 92. 36.77 0.04 2156700500017 93. 37.12 0.08 2156700500018 137. 53.20 0.03 2156700500019 138. 53.20 0.03 2156700500020 139. 54.42 0.11 2156700500021 140. 54.88 0.10 2156700500022 141. 54.88 0.10 2156700500023 142. 55.29 0.08 2156700500024 ENDDATA 15 0 2156700500025 ENDSUBENT 24 0 2156700599999 SUBENT 21567006 20160725 22522156700600001 BIB 2 2 2156700600002 REACTION (92-U-238(N,F)ELEM,,AP) Most probable mass. 2156700600003 STATUS (TABLE) Tables 9-2 (p.75), and 9-10 (p.85), Thesis. 2156700600004 ENDBIB 2 0 2156700600005 NOCOMMON 0 0 2156700600006 DATA 3 4 2156700600007 ELEMENT DATA DATA-ERR 2156700600008 NO-DIM NO-DIM NO-DIM 2156700600009 35. 87.60 0.20 2156700600010 36. 90.47 0.10 2156700600011 53. 136.40 0.10 2156700600012 54. 139.11 0.20 2156700600013 ENDDATA 6 0 2156700600014 ENDSUBENT 13 0 2156700699999 SUBENT 21567007 20160725 22522156700700001 BIB 2 2 2156700700002 REACTION (90-TH-232(N,F)ELEM,,AP) Most probable mass. 2156700700003 STATUS (TABLE) Table 9-2 (p.75) and 9-10 (p.85), Thesis. 2156700700004 ENDBIB 2 0 2156700700005 NOCOMMON 0 0 2156700700006 DATA 4 4 2156700700007 ELEMENT DATA +DATA-ERR -DATA-ERR 2156700700008 NO-DIM NO-DIM NO-DIM NO-DIM 2156700700009 35. 87.50 0.20 0.30 2156700700010 36. 90.26 0.10 0.10 2156700700011 53. 136.20 0.20 0.30 2156700700012 54. 139.06 0.15 0.15 2156700700013 ENDDATA 6 0 2156700700014 ENDSUBENT 13 0 2156700799999 SUBENT 21567008 20160725 22522156700800001 BIB 3 3 2156700800002 REACTION (90-TH-232(N,F),PR,NU) 2156700800003 STATUS (TABLE) Text, p.75, Thesis. 2156700800004 HISTORY (20160725A) SD: Data units were changed. 2156700800005 ENDBIB 3 0 2156700800006 NOCOMMON 0 0 2156700800007 DATA 2 1 2156700800008 DATA DATA-ERR 2156700800009 PRT/FIS PRT/FIS 2156700800010 3.68 0.18 2156700800011 ENDDATA 3 0 2156700800012 ENDSUBENT 11 0 2156700899999 ENDENTRY 8 0 2156799999999