ENTRY 40965 20200922 41894096500000001 SUBENT 40965001 20200922 41894096500100001 BIB 10 32 4096500100002 TITLE Difference of the angular distributions for fission 4096500100003 fragments of different masses in nuclear fission 4096500100004 AUTHOR (B.M.Gokhberg,L.D.Kozlov,S.K.Lisin,L.N.Morozov, 4096500100005 V.A.Pchelin,L.V.Chistyakov,V.A.Shigin, 4096500100006 V.M.Shubko,Yu.A.Yashin) 4096500100007 INSTITUTE (4RUSKUR) 4096500100008 REFERENCE (J,YF,47,320,1988) Iss.2. Main reference. 4096500100009 Data Table is given. 4096500100010 (J,SNP,47,201,1988) Engl.transl.of YF,47,320,1988 4096500100011 (J,YF,33,313,1981) Issue 2. 4096500100012 (J,SNP,33,165,1981) 4096500100013 Prelim.publication for U-238 data in Table. 4096500100014 INC-SOURCE (P-T) Monoenergetic neutrons. 4096500100015 Neutron beam 5.E+8 1/s/cm**2 . 4096500100016 FACILITY (VDG,4RUSKUR) Electrostatic accelerator 4096500100017 METHOD (CHSEP) 4096500100018 (STTA) Stack-target irradiation during 1-2 days. 4096500100019 DETECTOR (PLATE) For fission fragments detection. 4096500100020 (PROPC) Low-background 4PI beta counter - for fission 4096500100021 fragments activity measurements. 4096500100022 CORRECTION Correction was made on beta rays absorption 4096500100023 in the fission-fragment-containing sample 4096500100024 HISTORY (20030630C) Compiled at the CJD 4096500100025 (20030701U) Last checking has been done. 4096500100026 (20130812A) M.M. Upper -> lower case correction. 4096500100027 PRE code was removed in Subents 002-005. 4096500100028 PRE -> CUM in Subents 006-010. 4096500100029 (20200515A) Entry was corrected according to comments 4096500100030 of N.Otsuka (NDS,IAEA). 4096500100031 (20200922A) Refs. YF,33,313,1981 and Engl.translation 4096500100032 were added. REACTION was corrected in Subents 006,008, 4096500100033 010 . Minor correction of free text. 4096500100034 ENDBIB 32 0 4096500100035 COMMON 1 3 4096500100036 EN-RSL-HW 4096500100037 KEV 4096500100038 70. 4096500100039 ENDCOMMON 3 0 4096500100040 ENDSUBENT 39 0 4096500199999 SUBENT 40965002 20200922 41894096500200001 BIB 6 14 4096500200002 REACTION (90-TH-232(N,F),,DA,FF,RSD/MSC) 4096500200003 Angular anisotropy is integrated over all fission 4096500200004 fragments and is practically equal to the anisotropy 4096500200005 of the most-probable fission fragments (comment of 4096500200006 authors in Sov.Nucl.Phys.,v.47,p.201,1988) . 4096500200007 MONITOR No information 4096500200008 SAMPLE Metallic foils of fissionable material 0.1 mm thick 4096500200009 alternating with polystyrene plates (4.5 mg/cm2). 4096500200010 Collimators 3*3 cm2. All gathered in block 3*3*3 cm3. 4096500200011 Collimators were bronze plates 0.6 mm thick 4096500200012 MISC-COL (MISC) Number of irradiations 4096500200013 STATUS (TABLE) Column 4 of the Table 1 in 4096500200014 J.Sov.Nucl.Phys.,v.47,p.201,1988 4096500200015 HISTORY (20200515A) Code MSC was added. 4096500200016 ENDBIB 14 0 4096500200017 COMMON 1 3 4096500200018 ANG 4096500200019 ADEG 4096500200020 0. 4096500200021 ENDCOMMON 3 0 4096500200022 DATA 3 2 4096500200023 EN DATA MISC 4096500200024 MEV NO-DIM NO-DIM 4096500200025 1.58 0.4 10. 4096500200026 1.42 0.8 13. 4096500200027 ENDDATA 4 0 4096500200028 ENDSUBENT 27 0 4096500299999 SUBENT 40965003 20200922 41894096500300001 BIB 6 14 4096500300002 REACTION (92-U-238(N,F),,DA,FF,RSD/MSC) 4096500300003 Angular anisotropy is integrated over all fission 4096500300004 fragments and is practically equal to the anisotropy 4096500300005 of the most-probable fission fragments (comment of 4096500300006 authors in Sov.Nucl.Phys.,v.47,p.201,1988) . 4096500300007 MONITOR No information 4096500300008 SAMPLE Metallic foils of fissionable material 0.1 mm thick 4096500300009 alternating with polystyrene plates (4.5 mg/cm2). 4096500300010 Collimators 3*3 cm2.All gathered in block 3*3*3 cm3. 4096500300011 Collimators were bronze plates 0.6 mm thick. 4096500300012 MISC-COL (MISC) Number of irradiations 4096500300013 STATUS (TABLE) Column 4 of the Table 1 in 4096500300014 J.Sov.Nucl.Phys.,v.47,p.201,1988 4096500300015 HISTORY (20200515A) Code MSC was added. 4096500300016 ENDBIB 14 0 4096500300017 COMMON 1 3 4096500300018 ANG 4096500300019 ADEG 4096500300020 0. 4096500300021 ENDCOMMON 3 0 4096500300022 DATA 3 1 4096500300023 EN DATA MISC 4096500300024 MEV NO-DIM NO-DIM 4096500300025 1.55 1.5 15. 4096500300026 ENDDATA 3 0 4096500300027 ENDSUBENT 26 0 4096500399999 SUBENT 40965004 20200922 41894096500400001 BIB 6 14 4096500400002 REACTION (92-U-236(N,F),,DA,FF,RSD/MSC) 4096500400003 Angular anisotropy is integrated over all fission 4096500400004 fragments and is practically equal to the anisotropy 4096500400005 of the most-probable fission fragments (comment of 4096500400006 authors in Sov.Nucl.Phys.,v.47,p.201,1988) . 4096500400007 MONITOR No information 4096500400008 SAMPLE Aluminium foils with U-236 oxide layers on both sides 4096500400009 alternating with polystyrene plates (4.5 mg/cm2). 4096500400010 Collimators 3*3 cm2.All gathered in block 3*3*3 cm3. 4096500400011 Collimators were bronze plates 0.6 mm thick 4096500400012 MISC-COL (MISC) Number of irradiations 4096500400013 STATUS (TABLE) Column 4 of the Table 1 in 4096500400014 J.Sov.Nucl.Phys.,v.47,p.201,1988 4096500400015 HISTORY (20200515A) Code MSC was added. 4096500400016 ENDBIB 14 0 4096500400017 COMMON 1 3 4096500400018 ANG 4096500400019 ADEG 4096500400020 0. 4096500400021 ENDCOMMON 3 0 4096500400022 DATA 3 2 4096500400023 EN DATA MISC 4096500400024 MEV NO-DIM NO-DIM 4096500400025 1.25 1.45 16. 4096500400026 0.9 0.65 9. 4096500400027 ENDDATA 4 0 4096500400028 ENDSUBENT 27 0 4096500499999 SUBENT 40965005 20200922 41894096500500001 BIB 5 14 4096500500002 REACTION ((92-U-238(N,F)ELEM/MASS,CUM,DA,,RSD)/ 4096500500003 (92-U-238(N,F),,DA,FF,RSD/MSC)) Angular 4096500500004 anisotropy of a peculiar fragment is given relative 4096500500005 to the most probable fission-mode anisotropy 4096500500006 SAMPLE Metallic foils of fissionable material 0.1 mm thick 4096500500007 alternating with polystyrene plates(4.5 mg/cm2) 4096500500008 and collimators 3*3 cm2 All Gathered in block 4096500500009 3*3*3 cm3. Collimators were bronze plates 0.6 mm thick4096500500010 ERR-ANALYS (ERR-S) Statistical error 4096500500011 STATUS (TABLE) Columns 6-10 of the Table 1 in 4096500500012 J.Sov.Nucl.Phys.,v.47,p.201,1988. 4096500500013 = last line in Table of Yad.Fiz.,v.33,p.313,1981 4096500500014 (DEP,40965003) most probable anisotropy 4096500500015 HISTORY (20200515A) CUM and MSC codes were added. 4096500500016 ENDBIB 14 0 4096500500017 COMMON 2 3 4096500500018 EN ANG 4096500500019 MEV ADEG 4096500500020 1.55 0. 4096500500021 ENDCOMMON 3 0 4096500500022 DATA 4 5 4096500500023 ELEMENT MASS DATA ERR-S 4096500500024 NO-DIM NO-DIM NO-DIM NO-DIM 4096500500025 38. 89. 1.01 0.03 4096500500026 47. 111. 1.04 0.05 4096500500027 48. 115. 1.02 0.08 4096500500028 51. 127. 1.1 0.05 4096500500029 51. 129. 1.09 0.09 4096500500030 ENDDATA 7 0 4096500500031 ENDSUBENT 30 0 4096500599999 SUBENT 40965006 20200922 41894096500600001 BIB 4 17 4096500600002 REACTION (((92-U-238(N,F)56-BA-140,CUM,FY,,FCT)+ 4096500600003 (92-U-238(N,F)42-MO-99,CUM,FY,,FCT))/ 4096500600004 (92-U-238(N,F)ELEM/MASS,CUM,FY)) FCT=0.5. 4096500600005 Ratio of most probable yield ( = half of sum of Ba-1404096500600006 and Mo-99 yields) to yield of specified isotope. 4096500600007 SAMPLE Metallic foils of fissionable material 0.1 mm thick 4096500600008 alternating with polystyrene plates (4.5 mg/cm2) 4096500600009 and collimators 3*3 cm2.All gathered in block 4096500600010 3*3*3 cm3. Collimators were bronze plates 0.6 mm thick4096500600011 STATUS (TABLE) Columns 6-10 of the Table 1 in 4096500600012 J.Sov.Nucl.Phys.,v.47,p.201,1988 4096500600013 Directly measured ratio values are given in Table 4096500600014 of Yad.Fiz.,v.33,p.313,1981 for angles 0 and 90 deg. 4096500600015 HISTORY (20200515A) Reaction was corrected. 4096500600016 (20200922A) FCT code was added in REACTION 4096500600017 according to comment of authors in 4096500600018 Yad.Fiz.,v.33,p.313,1981, page 316. 4096500600019 ENDBIB 17 0 4096500600020 COMMON 1 3 4096500600021 EN 4096500600022 MEV 4096500600023 1.55 4096500600024 ENDCOMMON 3 0 4096500600025 DATA 3 5 4096500600026 ELEMENT MASS DATA 4096500600027 NO-DIM NO-DIM NO-DIM 4096500600028 38. 89. 4.9 4096500600029 47. 111. 238. 4096500600030 48. 115. 730. 4096500600031 51. 127. 126. 4096500600032 51. 129. 23. 4096500600033 ENDDATA 7 0 4096500600034 ENDSUBENT 33 0 4096500699999 SUBENT 40965007 20200515 41874096500700001 BIB 5 13 4096500700002 REACTION ((92-U-236(N,F)ELEM/MASS,CUM,DA,,RSD)/ 4096500700003 (92-U-236(N,F),,DA,FF,RSD/MSC)) Angular 4096500700004 anisotropy of a peculiar fragment is given relative 4096500700005 to the most probable fission-mode anisotropy 4096500700006 SAMPLE .Aluminium foils with U-236 oxide layers on both sides 4096500700007 alternating with polystyrene plates (4.5 mg/cm2). 4096500700008 Collimators 3*3 cm2.All gathered in block 3*3*3 cm3. 4096500700009 Collimators were bronze plates 0.6 mm thick 4096500700010 ERR-ANALYS (ERR-S) Statistical error 4096500700011 STATUS (TABLE) Columns 6-10 of the Table 1 in 4096500700012 J.Sov.Nucl.Phys.,v.47,p.201,1988 4096500700013 (DEP,40965004) 4096500700014 HISTORY (20200515A) Code MSC was added. 4096500700015 ENDBIB 13 0 4096500700016 COMMON 1 3 4096500700017 ANG 4096500700018 ADEG 4096500700019 0. 4096500700020 ENDCOMMON 3 0 4096500700021 DATA 5 8 4096500700022 EN ELEMENT MASS DATA ERR-S 4096500700023 MEV NO-DIM NO-DIM NO-DIM NO-DIM 4096500700024 1.25 38. 89. 0.96 0.06 4096500700025 1.25 47. 111. 1.05 0.07 4096500700026 1.25 48. 115. 1.09 0.08 4096500700027 1.25 51. 127. 0.98 0.16 4096500700028 1.25 51. 129. 1.07 0.14 4096500700029 0.9 38. 89. 0.95 0.05 4096500700030 0.9 51. 127. 1.14 0.085 4096500700031 0.9 51. 129. 1.19 0.13 4096500700032 ENDDATA 10 0 4096500700033 ENDSUBENT 32 0 4096500799999 SUBENT 40965008 20200922 41894096500800001 BIB 4 15 4096500800002 REACTION (((92-U-236(N,F)56-BA-140,CUM,FY,,FCT)+ 4096500800003 (92-U-236(N,F)42-MO-99,CUM,FY,,FCT))/ 4096500800004 (92-U-236(N,F)ELEM/MASS,CUM,FY)) FCT=0.5 4096500800005 Ratio of most probable yield ( = half of sum of Ba-1404096500800006 and Mo-99 yields) to yield of specified isotope. 4096500800007 SAMPLE Metallic foils of fissionable material 0.1 mm thick 4096500800008 alternating with polystyrene plates (4.5 mg/cm2) 4096500800009 and collimators 3*3 cm2.All gathered in block 4096500800010 3*3*3 cm3. Collimators were bronze plates 0.6 mm thick4096500800011 STATUS (TABLE) Columns 6-10 of the Table 1 in 4096500800012 J.Sov.Nucl.Phys.,v.47,p.201,1988 4096500800013 HISTORY (20200515A) Reaction was corrected. 4096500800014 (20200922A) FCT code was added in REACTION 4096500800015 according to comment of authors (for U-238 data) in 4096500800016 Yad.Fiz.,v.33,p.313,1981, page 316. 4096500800017 ENDBIB 15 0 4096500800018 NOCOMMON 0 0 4096500800019 DATA 4 8 4096500800020 EN ELEMENT MASS DATA 4096500800021 MEV NO-DIM NO-DIM NO-DIM 4096500800022 1.25 38. 89. 3.4 4096500800023 1.25 47. 111. 332. 4096500800024 1.25 48. 115. 416. 4096500800025 1.25 51. 127. 63. 4096500800026 1.25 51. 129. 11. 4096500800027 0.9 38. 89. 3.3 4096500800028 0.9 51. 127. 78. 4096500800029 0.9 51. 129. 10. 4096500800030 ENDDATA 10 0 4096500800031 ENDSUBENT 30 0 4096500899999 SUBENT 40965009 20200515 41874096500900001 BIB 5 13 4096500900002 REACTION ((90-TH-232(N,F)51-SB-129,CUM,DA,,RSD)/ 4096500900003 (90-TH-232(N,F),,DA,FF,RSD/MSC)) Angular 4096500900004 anisotropy of a peculiar fragment is given relative 4096500900005 to the most probable fission-mode anisotropy 4096500900006 SAMPLE .Metallic foils of fissionable material 0.1 mm thick 4096500900007 alternating with polystyrene plates (4.5 mg/cm2). 4096500900008 Collimators 3*3 cm2. All gathered in block 3*3*3 cm3. 4096500900009 Collimators were bronze plates 0.6 mm thick 4096500900010 ERR-ANALYS (ERR-S) Statistical error 4096500900011 STATUS (TABLE) Column 10 of the Table 1 in 4096500900012 J.Sov.Nucl.Phys.,v.47,p.201,1988 4096500900013 (DEP,40965002) 4096500900014 HISTORY (20200515A) Code MSC was added. 4096500900015 ENDBIB 13 0 4096500900016 COMMON 1 3 4096500900017 ANG 4096500900018 ADEG 4096500900019 0. 4096500900020 ENDCOMMON 3 0 4096500900021 DATA 3 2 4096500900022 EN DATA ERR-S 4096500900023 MEV NO-DIM NO-DIM 4096500900024 1.58 1.160 0.055 4096500900025 1.42 1.086 0.043 4096500900026 ENDDATA 4 0 4096500900027 ENDSUBENT 26 0 4096500999999 SUBENT 40965010 20200922 41894096501000001 BIB 4 16 4096501000002 REACTION (((90-TH-232(N,F)56-BA-140,CUM,FY,,FCT)+ 4096501000003 (90-TH-232(N,F)42-MO-99,CUM,FY,,FCT))/ 4096501000004 (90-TH-232(N,F)51-SB-129,CUM,FY)) FCT=0.5 4096501000005 Ratio of most probable yield ( = half of sum of Ba-1404096501000006 and Mo-99 yields) to yield of specified isotope. 4096501000007 SAMPLE Metallic foils of fissionable material 0.1 mm thick 4096501000008 alternating with polystyrene plates (4.5 mg/cm2) 4096501000009 and collimators 3*3 cm2. All gathered in block. 4096501000010 3*3*3 cm3. Collimators were bronze plates 0.6 mm thick4096501000011 STATUS (TABLE) Column 10 of the Table 1 in 4096501000012 J.Sov.Nucl.Phys.,v.47,p.201,1988 4096501000013 values are given as 1/63, 1/62 . 4096501000014 HISTORY (20200515A) Reaction was corrected. 4096501000015 (20200922A) FCT code was added in REACTION 4096501000016 according to comment of authors (for U-238 data) in 4096501000017 Yad.Fiz.,v.33,p.313,1981, page 316. 4096501000018 ENDBIB 16 0 4096501000019 NOCOMMON 0 0 4096501000020 DATA 2 2 4096501000021 EN DATA 4096501000022 MEV NO-DIM 4096501000023 1.58 63. 4096501000024 1.42 62. 4096501000025 ENDDATA 4 0 4096501000026 ENDSUBENT 25 0 4096501099999 ENDENTRY 10 0 4096599999999