ENTRY O0992 20040321 0000O099200000001 SUBENT O0992001 20040321 0000O099200100001 BIB 10 50 O099200100002 TITLE Fission induced in U-nat, Pb-nat, Au-197 and Ho-165 O099200100003 by 80 and 100-MeV pi+ and pi-. O099200100004 AUTHOR (H.A.Khan, N.A.Khan, R.J.Peterson) O099200100005 INSTITUTE (3PAKNIL) O099200100006 (3PAKPAK) Nuclear Physical Standards Laboratories. O099200100007 (1USACOL) Nuclear Physics Laboratory. O099200100008 REFERENCE (J,PR/C,35,645,1987) O099200100009 HISTORY (20030906C) O099200100010 (20040321U) Last checking has been done. O099200100011 ADD-RES (COMP) The results have been compared with the scanty O099200100012 data available on the subject and with systems having O099200100013 comparable excitation energies. O099200100014 Angular correlation of the reaction products have been O099200100015 obtained. O099200100016 SAMPLE Target layers of spectroscopically pure natural O099200100017 uranium, lead, gold and holmium were deposited on the O099200100018 selected detectors. The target thickness deposited O099200100019 varied from about 300-mum/cm**2 to about 1.15 mg/cm**2,O099200100020 as determined by weighing before and after deposition. O099200100021 These thickness are known to 7% or better. O099200100022 DETECTOR (TRD) Seven type of solid state nuclear track O099200100023 detector, having different charge thresholds was used. O099200100024 It is CR-39, CN-85, Makrofoil E, lexan, Muscovite mica,O099200100025 Phosphate glass, Soda lime glass. O099200100026 Careful selection of the detectors was made before O099200100027 target deposition. Detectors not previously exposed to O099200100028 the laboratory environment and having clean surfaces O099200100029 were taken out of a stock of detectors reserved at O099200100030 freezing temperatures. Muscovite mica detectors were O099200100031 used after exposing freshly peeled-off layers. Mica O099200100032 registers only the heavy products. O099200100033 Track detectors of CR-39 registers both light and heavyO099200100034 products. O099200100035 METHOD (STTA) O099200100036 (CHSEP) O099200100037 ERR-ANALYS The muon contamination of the pion beam is less than O099200100038 20%. This contamination is not expected to contribute O099200100039 more than 2% to the fission cross section when comparedO099200100040 to electrofission cross sections at the same momentum. O099200100041 The fission contribution of an electron component O099200100042 present in the beam is estimated to be less than 2%. O099200100043 The contribution due to the proton contamination was O099200100044 eliminated altogether by using an absorber in the beam O099200100045 of pions. The contribution of these neutrons in the O099200100046 U-natural fission cross section has been estimated to O099200100047 be less than 3%. These contributions of slow and fast O099200100048 neutrons were confirmed by Bonner sphere measurements O099200100049 and the fission rate measurements when the target O099200100050 detector assemblies were displaced away from the pion O099200100051 beam. O099200100052 ENDBIB 50 0 O099200100053 NOCOMMON 0 0 O099200100054 ENDSUBENT 53 0 O099200199999 SUBENT O0992002 20040321 0000O099200200001 BIB 3 6 O099200200002 REACTION 1(92-U-0(PIN,F),BIN,SIG) O099200200003 2(92-U-0(PIN,F),TER,SIG) O099200200004 STATUS (TABLE) O099200200005 ERR-ANALYS (ERR-S) It is the statistical accuracy only. O099200200006 (ERR-1) Other sources of uncertainty in magnitude, as O099200200007 already discussed, have been estimated to be about 20%.O099200200008 ENDBIB 6 0 O099200200009 COMMON 1 3 O099200200010 ERR-1 O099200200011 PER-CENT O099200200012 20. O099200200013 ENDCOMMON 3 0 O099200200014 DATA 5 2 O099200200015 EN DATA 1ERR-S 1DATA 2ERR-S 2 O099200200016 MEV MB MB MB MB O099200200017 80. 2890. 54. 15. 4. O099200200018 100. 2260. 48. 13. 4. O099200200019 ENDDATA 4 0 O099200200020 ENDSUBENT 19 0 O099200299999 SUBENT O0992003 20040321 0000O099200300001 BIB 3 6 O099200300002 REACTION 1(92-U-0(PIP,F),BIN,SIG) O099200300003 2(92-U-0(PIP,F),TER,SIG) O099200300004 STATUS (TABLE) O099200300005 ERR-ANALYS (ERR-S) It is the statistical accuracy only. O099200300006 (ERR-1) Other sources of uncertainty in magnitude, as O099200300007 already discussed, have been estimated to be about 20%.O099200300008 ENDBIB 6 0 O099200300009 COMMON 1 3 O099200300010 ERR-1 O099200300011 PER-CENT O099200300012 20. O099200300013 ENDCOMMON 3 0 O099200300014 DATA 5 1 O099200300015 EN DATA 1ERR-S 1DATA 2ERR-S 2 O099200300016 MEV MB MB MB MB O099200300017 80. 2020. 45. 11. 4. O099200300018 ENDDATA 3 0 O099200300019 ENDSUBENT 18 0 O099200399999 SUBENT O0992004 20040321 0000O099200400001 BIB 3 6 O099200400002 REACTION 1(82-PB-0(PIP,F),BIN,SIG) O099200400003 2(82-PB-0(PIP,F),TER,SIG) O099200400004 STATUS (TABLE) O099200400005 ERR-ANALYS (ERR-S) It is the statistical accuracy only. O099200400006 (ERR-1) Other sources of uncertainty in magnitude, as O099200400007 already discussed, have been estimated to be about 20%.O099200400008 ENDBIB 6 0 O099200400009 COMMON 1 3 O099200400010 ERR-1 O099200400011 PER-CENT O099200400012 20. O099200400013 ENDCOMMON 3 0 O099200400014 DATA 5 2 O099200400015 EN DATA 1ERR-S 1DATA 2ERR-S 2 O099200400016 MEV MB MB MB MB O099200400017 80. 260. 17. 1. 1. O099200400018 100. 258. 16. 2. 1. O099200400019 ENDDATA 4 0 O099200400020 ENDSUBENT 19 0 O099200499999 SUBENT O0992005 20040321 0000O099200500001 BIB 3 5 O099200500002 REACTION (79-AU-197(PIP,F),BIN,SIG) O099200500003 STATUS (TABLE) O099200500004 ERR-ANALYS (ERR-S) It is the statistical accuracy only. O099200500005 (ERR-1) Other sources of uncertainty in magnitude, as O099200500006 already discussed, have been estimated to be about 20%.O099200500007 ENDBIB 5 0 O099200500008 COMMON 1 3 O099200500009 ERR-1 O099200500010 PER-CENT O099200500011 20. O099200500012 ENDCOMMON 3 0 O099200500013 DATA 3 2 O099200500014 EN DATA ERR-S O099200500015 MEV MB MB O099200500016 80. 79. 9. O099200500017 100. 81. 9. O099200500018 ENDDATA 4 0 O099200500019 ENDSUBENT 18 0 O099200599999 SUBENT O0992006 20040321 0000O099200600001 BIB 3 5 O099200600002 REACTION (67-HO-165(PIP,F),BIN,SIG) O099200600003 STATUS (TABLE) O099200600004 ERR-ANALYS (ERR-S) It is the statistical accuracy only. O099200600005 (ERR-1) Other sources of uncertainty in magnitude, as O099200600006 already discussed, have been estimated to be about 20%.O099200600007 ENDBIB 5 0 O099200600008 COMMON 1 3 O099200600009 ERR-1 O099200600010 PER-CENT O099200600011 20. O099200600012 ENDCOMMON 3 0 O099200600013 DATA 3 2 O099200600014 EN DATA ERR-S O099200600015 MEV MB MB O099200600016 80. 3. 2. O099200600017 100. 4. 2. O099200600018 ENDDATA 4 0 O099200600019 ENDSUBENT 18 0 O099200699999 SUBENT O0992007 20040321 0000O099200700001 BIB 4 15 O099200700002 REACTION (92-U-0(PIP,F),,DA,LF,REL) Fig.2 O099200700003 STATUS (CURVE) By CAJAD. O099200700004 COMMENT -By authors. 1. The 4-pi geometry detector arrangementsO099200700005 were analyzed to determine the differential angular O099200700006 cross section distributions for the emission of light O099200700007 products and the heavy fission fragments. O099200700008 2. Fission fragment distribution have been normalized aO099200700009 relative value of 2.5 for angular interval of 0-10 O099200700010 degrees for the target. O099200700011 The angular distributions of the fission fragments and O099200700012 of the light reaction products in different angular O099200700013 intervals have been plotted relative to this normalizedO099200700014 value. O099200700015 ERR-ANALYS (DATA-ERR) The uncertainty is shown on figures, withoutO099200700016 any analysis. O099200700017 ENDBIB 15 0 O099200700018 COMMON 1 3 O099200700019 EN O099200700020 MEV O099200700021 80. O099200700022 ENDCOMMON 3 0 O099200700023 DATA 4 9 O099200700024 ANG-MIN ANG-MAX DATA DATA-ERR O099200700025 ADEG ADEG ARB-UNITS ARB-UNITS O099200700026 0. 10. 6.24 0.25 O099200700027 10. 20. 5.86 0.23 O099200700028 20. 30. 6.03 0.21 O099200700029 30. 40. 5.88 0.21 O099200700030 40. 50. 5.78 0.21 O099200700031 50. 60. 5.63 0.23 O099200700032 60. 70. 5.79 0.21 O099200700033 70. 80. 5.46 0.27 O099200700034 80. 90. 5.18 0.21 O099200700035 ENDDATA 11 0 O099200700036 ENDSUBENT 35 0 O099200799999 SUBENT O0992008 20040321 0000O099200800001 BIB 4 15 O099200800002 REACTION (92-U-0(PIP,F),,DA,FF,REL) Fig.2 O099200800003 STATUS (CURVE) By CAJAD. O099200800004 COMMENT -By authors. 1. The 4-pi geometry detector arrangementsO099200800005 were analyzed to determine the differential angular O099200800006 cross section distributions for the emission of light O099200800007 products and the heavy fission fragments. O099200800008 2. Fission fragment distribution have been normalized aO099200800009 relative value of 2.5 for angular interval of 0-10 O099200800010 degrees for the target. O099200800011 The angular distributions of the fission fragments and O099200800012 of the light reaction products in different angular O099200800013 intervals have been plotted relative to this normalizedO099200800014 value. O099200800015 ERR-ANALYS (DATA-ERR) The uncertainty is shown on figures, withoutO099200800016 any analysis. O099200800017 ENDBIB 15 0 O099200800018 COMMON 1 3 O099200800019 EN O099200800020 MEV O099200800021 80. O099200800022 ENDCOMMON 3 0 O099200800023 DATA 4 9 O099200800024 ANG-MIN ANG-MAX DATA DATA-ERR O099200800025 ADEG ADEG ARB-UNITS ARB-UNITS O099200800026 0. 10. 2.49 0.23 O099200800027 10. 20. 2.34 0.19 O099200800028 20. 30. 2.19 0.23 O099200800029 30. 40. 2.27 0.19 O099200800030 40. 50. 2.25 0.21 O099200800031 50. 60. 2.06 0.21 O099200800032 60. 70. 1.96 0.25 O099200800033 70. 80. 2.12 0.23 O099200800034 80. 90. 2.02 0.25 O099200800035 ENDDATA 11 0 O099200800036 ENDSUBENT 35 0 O099200899999 SUBENT O0992009 20040321 0000O099200900001 BIB 4 15 O099200900002 REACTION (82-PB-0(PIP,F),,DA,LF,REL) Fig.2 O099200900003 STATUS (CURVE) By CAJAD. O099200900004 COMMENT -By authors. 1. The 4-pi geometry detector arrangementsO099200900005 were analyzed to determine the differential angular O099200900006 cross section distributions for the emission of light O099200900007 products and the heavy fission fragments. O099200900008 2. Fission fragment distribution have been normalized aO099200900009 relative value of 2.5 for angular interval of 0-10 O099200900010 degrees for the target. O099200900011 The angular distributions of the fission fragments and O099200900012 of the light reaction products in different angular O099200900013 intervals have been plotted relative to this normalizedO099200900014 value. O099200900015 ERR-ANALYS (DATA-ERR) The uncertainty is shown on figures, withoutO099200900016 any analysis. O099200900017 ENDBIB 15 0 O099200900018 COMMON 1 3 O099200900019 EN O099200900020 MEV O099200900021 80. O099200900022 ENDCOMMON 3 0 O099200900023 DATA 4 9 O099200900024 ANG-MIN ANG-MAX DATA DATA-ERR O099200900025 ADEG ADEG ARB-UNITS ARB-UNITS O099200900026 0. 10. 5.22 0.25 O099200900027 10. 20. 5. 0.23 O099200900028 20. 30. 5.13 0.23 O099200900029 30. 40. 4.96 0.25 O099200900030 40. 50. 4.96 0.27 O099200900031 50. 60. 4.9 0.3 O099200900032 60. 70. 4.74 0.27 O099200900033 70. 80. 4.65 0.25 O099200900034 80. 90. 4.52 0.27 O099200900035 ENDDATA 11 0 O099200900036 ENDSUBENT 35 0 O099200999999 SUBENT O0992010 20040321 0000O099201000001 BIB 4 15 O099201000002 REACTION (82-PB-0(PIP,F),,DA,FF,REL) Fig.2 O099201000003 STATUS (CURVE) By CAJAD. O099201000004 COMMENT -By authors. 1. The 4-pi geometry detector arrangementsO099201000005 were analyzed to determine the differential angular O099201000006 cross section distributions for the emission of light O099201000007 products and the heavy fission fragments. O099201000008 2. Fission fragment distribution have been normalized aO099201000009 relative value of 2.5 for angular interval of 0-10 O099201000010 degrees for the target. O099201000011 The angular distributions of the fission fragments and O099201000012 of the light reaction products in different angular O099201000013 intervals have been plotted relative to this normalizedO099201000014 value. O099201000015 ERR-ANALYS (DATA-ERR) The uncertainty is shown on figures, withoutO099201000016 any analysis. O099201000017 ENDBIB 15 0 O099201000018 COMMON 1 3 O099201000019 EN O099201000020 MEV O099201000021 80. O099201000022 ENDCOMMON 3 0 O099201000023 DATA 4 9 O099201000024 ANG-MIN ANG-MAX DATA DATA-ERR O099201000025 ADEG ADEG ARB-UNITS ARB-UNITS O099201000026 0. 10. 2.59 0.23 O099201000027 10. 20. 2.24 0.16 O099201000028 20. 30. 2.37 0.16 O099201000029 30. 40. 2.15 0.25 O099201000030 40. 50. 2.15 0.23 O099201000031 50. 60. 1.97 0.25 O099201000032 60. 70. 2.06 0.23 O099201000033 70. 80. 1.93 0.23 O099201000034 80. 90. 1.89 0.23 O099201000035 ENDDATA 11 0 O099201000036 ENDSUBENT 35 0 O099201099999 SUBENT O0992011 20040321 0000O099201100001 BIB 4 15 O099201100002 REACTION (79-AU-197(PIP,F),,DA,LF,REL) Fig.2 O099201100003 STATUS (CURVE) By CAJAD. O099201100004 COMMENT -By authors. 1. The 4-pi geometry detector arrangementsO099201100005 were analyzed to determine the differential angular O099201100006 cross section distributions for the emission of light O099201100007 products and the heavy fission fragments. O099201100008 2. Fission fragment distribution have been normalized aO099201100009 relative value of 2.5 for angular interval of 0-10 O099201100010 degrees for the target. O099201100011 The angular distributions of the fission fragments and O099201100012 of the light reaction products in different angular O099201100013 intervals have been plotted relative to this normalizedO099201100014 value. O099201100015 ERR-ANALYS (DATA-ERR) The uncertainty is shown on figures, withoutO099201100016 any analysis. O099201100017 ENDBIB 15 0 O099201100018 COMMON 1 3 O099201100019 EN O099201100020 MEV O099201100021 80. O099201100022 ENDCOMMON 3 0 O099201100023 DATA 4 9 O099201100024 ANG-MIN ANG-MAX DATA DATA-ERR O099201100025 ADEG ADEG ARB-UNITS ARB-UNITS O099201100026 0. 10. 4.8 0.23 O099201100027 10. 20. 4.67 0.15 O099201100028 20. 30. 4.53 0.19 O099201100029 30. 40. 4.67 0.23 O099201100030 40. 50. 4.58 0.25 O099201100031 50. 60. 4.44 0.25 O099201100032 60. 70. 4.49 0.3 O099201100033 70. 80. 4.22 0.27 O099201100034 80. 90. 4.1 0.3 O099201100035 ENDDATA 11 0 O099201100036 ENDSUBENT 35 0 O099201199999 SUBENT O0992012 20040321 0000O099201200001 BIB 4 15 O099201200002 REACTION (79-AU-197(PIP,F),,DA,FF,REL) Fig.2 O099201200003 STATUS (CURVE) By CAJAD. O099201200004 COMMENT -By authors. 1. The 4-pi geometry detector arrangementsO099201200005 were analyzed to determine the differential angular O099201200006 cross section distributions for the emission of light O099201200007 products and the heavy fission fragments. O099201200008 2. Fission fragment distribution have been normalized aO099201200009 relative value of 2.5 for angular interval of 0-10 O099201200010 degrees for the target. O099201200011 The angular distributions of the fission fragments and O099201200012 of the light reaction products in different angular O099201200013 intervals have been plotted relative to this normalizedO099201200014 value. O099201200015 ERR-ANALYS (DATA-ERR) The uncertainty is shown on figures, withoutO099201200016 any analysis. O099201200017 ENDBIB 15 0 O099201200018 COMMON 1 3 O099201200019 EN O099201200020 MEV O099201200021 80. O099201200022 ENDCOMMON 3 0 O099201200023 DATA 4 9 O099201200024 ANG-MIN ANG-MAX DATA DATA-ERR O099201200025 ADEG ADEG ARB-UNITS ARB-UNITS O099201200026 0. 10. 2.62 0.21 O099201200027 10. 20. 2.18 0.17 O099201200028 20. 30. 2.27 0.19 O099201200029 30. 40. 2.31 0.25 O099201200030 40. 50. 2.31 0.23 O099201200031 50. 60. 2. 0.3 O099201200032 60. 70. 2.09 0.23 O099201200033 70. 80. 1.91 0.23 O099201200034 80. 90. 1.73 0.23 O099201200035 ENDDATA 11 0 O099201200036 ENDSUBENT 35 0 O099201299999 SUBENT O0992013 20040321 0000O099201300001 BIB 4 15 O099201300002 REACTION (67-HO-165(PIP,F),,DA,LF,REL) Fig.2 O099201300003 STATUS (CURVE) By CAJAD. O099201300004 COMMENT -By authors. 1. The 4-pi geometry detector arrangementsO099201300005 were analyzed to determine the differential angular O099201300006 cross section distributions for the emission of light O099201300007 products and the heavy fission fragments. O099201300008 2. Fission fragment distribution have been normalized aO099201300009 relative value of 2.5 for angular interval of 0-10 O099201300010 degrees for the target. O099201300011 The angular distributions of the fission fragments and O099201300012 of the light reaction products in different angular O099201300013 intervals have been plotted relative to this normalizedO099201300014 value. O099201300015 ERR-ANALYS (DATA-ERR) The uncertainty is shown on figures, withoutO099201300016 any analysis. O099201300017 ENDBIB 15 0 O099201300018 COMMON 1 3 O099201300019 EN O099201300020 MEV O099201300021 80. O099201300022 ENDCOMMON 3 0 O099201300023 DATA 4 9 O099201300024 ANG-MIN ANG-MAX DATA DATA-ERR O099201300025 ADEG ADEG ARB-UNITS ARB-UNITS O099201300026 0. 10. 3.89 0.17 O099201300027 10. 20. 3.78 0.22 O099201300028 20. 30. 3.96 0.28 O099201300029 30. 40. 3.87 0.24 O099201300030 40. 50. 3.73 0.24 O099201300031 50. 60. 3.5 0.3 O099201300032 60. 70. 3.45 0.22 O099201300033 70. 80. 3.2 0.3 O099201300034 80. 90. 2.95 0.19 O099201300035 ENDDATA 11 0 O099201300036 ENDSUBENT 35 0 O099201399999 SUBENT O0992014 20040321 0000O099201400001 BIB 4 15 O099201400002 REACTION (67-HO-165(PIP,F),,DA,FF,REL) Fig.2 O099201400003 STATUS (CURVE) By CAJAD. O099201400004 COMMENT -By authors. 1. The 4-pi geometry detector arrangementsO099201400005 were analyzed to determine the differential angular O099201400006 cross section distributions for the emission of light O099201400007 products and the heavy fission fragments. O099201400008 2. Fission fragment distribution have been normalized aO099201400009 relative value of 2.5 for angular interval of 0-10 O099201400010 degrees for the target. O099201400011 The angular distributions of the fission fragments and O099201400012 of the light reaction products in different angular O099201400013 intervals have been plotted relative to this normalizedO099201400014 value. O099201400015 ERR-ANALYS (DATA-ERR) The uncertainty is shown on figures, withoutO099201400016 any analysis. O099201400017 ENDBIB 15 0 O099201400018 COMMON 1 3 O099201400019 EN O099201400020 MEV O099201400021 80. O099201400022 ENDCOMMON 3 0 O099201400023 DATA 4 9 O099201400024 ANG-MIN ANG-MAX DATA DATA-ERR O099201400025 ADEG ADEG ARB-UNITS ARB-UNITS O099201400026 0. 10. 2.58 0.17 O099201400027 10. 20. 2.58 0.24 O099201400028 20. 30. 2.3 0.26 O099201400029 30. 40. 2.21 0.24 O099201400030 40. 50. 1.98 0.26 O099201400031 50. 60. 2.03 0.24 O099201400032 60. 70. 1.93 0.17 O099201400033 70. 80. 1.89 0.19 O099201400034 80. 90. 1.56 0.19 O099201400035 ENDDATA 11 0 O099201400036 ENDSUBENT 35 0 O099201499999 SUBENT O0992015 20040321 0000O099201500001 BIB 4 7 O099201500002 REACTION (92-U-0(PIP,F),,DA,LF,REL) Fig.3 O099201500003 STATUS (CURVE) By CAJAD. O099201500004 FLAG (1.) CR-39 detector was used. O099201500005 (2.) CN-85 detector was used. O099201500006 (3.) Lexan detector was used. O099201500007 ERR-ANALYS (DATA-ERR) The uncertainty is shown on figures, withoutO099201500008 any analysis. O099201500009 ENDBIB 7 0 O099201500010 COMMON 1 3 O099201500011 EN O099201500012 MEV O099201500013 80. O099201500014 ENDCOMMON 3 0 O099201500015 DATA 5 27 O099201500016 ANG-MIN ANG-MAX DATA DATA-ERR FLAG O099201500017 ADEG ADEG ARB-UNITS ARB-UNITS NO-DIM O099201500018 0. 10. 12.27 0.19 1. O099201500019 0. 10. 6.13 0.19 2. O099201500020 0. 10. 5.38 0.17 3. O099201500021 10. 20. 11.91 0.15 1. O099201500022 10. 20. 6.27 0.15 2. O099201500023 10. 20. 5.24 0.19 3. O099201500024 20. 30. 12.18 0.21 1. O099201500025 20. 30. 5.38 0.23 3. O099201500026 20. 30. 6.09 0.23 2. O099201500027 30. 40. 11.87 0.11 1. O099201500028 30. 40. 6.22 0.19 2. O099201500029 30. 40. 5.2 0.21 3. O099201500030 40. 50. 11.82 0.21 1. O099201500031 40. 50. 5.91 0.17 2. O099201500032 40. 50. 5.02 0.15 3. O099201500033 50. 60. 11.87 0.21 1. O099201500034 50. 60. 5.73 0.19 2. O099201500035 50. 60. 4.93 0.21 3. O099201500036 60. 70. 11.6 0.19 1. O099201500037 60. 70. 5.82 0.19 2. O099201500038 60. 70. 4.98 0.19 3. O099201500039 70. 80. 11.29 0.23 1. O099201500040 70. 80. 5.47 0.17 2. O099201500041 70. 80. 4.89 0.21 3. O099201500042 80. 90. 5.24 0.15 2. O099201500043 80. 90. 11.07 0.17 1. O099201500044 80. 90. 4.8 0.17 3. O099201500045 ENDDATA 29 0 O099201500046 ENDSUBENT 45 0 O099201599999 SUBENT O0992016 20040321 0000O099201600001 BIB 4 7 O099201600002 REACTION (92-U-0(PIP,F),,DA,FF,REL) Fig.3 O099201600003 STATUS (CURVE) By CAJAD. O099201600004 COMMENT -By authors. The differential angular cross sections O099201600005 for fission fragments were obtained by using muscovite O099201600006 mica track detectors. O099201600007 ERR-ANALYS (DATA-ERR) The uncertainty is shown on figures, withoutO099201600008 any analysis. O099201600009 ENDBIB 7 0 O099201600010 COMMON 1 3 O099201600011 EN O099201600012 MEV O099201600013 80. O099201600014 ENDCOMMON 3 0 O099201600015 DATA 4 9 O099201600016 ANG-MIN ANG-MAX DATA DATA-ERR O099201600017 ADEG ADEG ARB-UNITS ARB-UNITS O099201600018 0. 10. 4.89 0.23 O099201600019 10. 20. 4.67 0.19 O099201600020 20. 30. 4.8 0.15 O099201600021 30. 40. 4.53 0.21 O099201600022 40. 50. 4.4 0.17 O099201600023 50. 60. 4.49 0.19 O099201600024 60. 70. 4.4 0.17 O099201600025 70. 80. 4.22 0.19 O099201600026 80. 90. 4. 0.21 O099201600027 ENDDATA 11 0 O099201600028 ENDSUBENT 27 0 O099201699999 SUBENT O0992017 20040321 0000O099201700001 BIB 4 7 O099201700002 REACTION (67-HO-165(PIP,F),,DA,LF,REL) Fig.3 O099201700003 STATUS (CURVE) By CAJAD. O099201700004 COMMENT -By authors. The differential angular cross sections O099201700005 for fission fragments were obtained by using CR-39 O099201700006 detectors. O099201700007 ERR-ANALYS (DATA-ERR) The uncertainty is shown on figures, withoutO099201700008 any analysis. O099201700009 ENDBIB 7 0 O099201700010 COMMON 1 3 O099201700011 EN O099201700012 MEV O099201700013 80. O099201700014 ENDCOMMON 3 0 O099201700015 DATA 4 9 O099201700016 ANG-MIN ANG-MAX DATA DATA-ERR O099201700017 ADEG ADEG ARB-UNITS ARB-UNITS O099201700018 0. 10. 8.23 0.3 O099201700019 10. 20. 8. 0.3 O099201700020 20. 30. 7.82 0.3 O099201700021 30. 40. 8.02 0.27 O099201700022 40. 50. 7.8 0.3 O099201700023 50. 60. 7.53 0.25 O099201700024 60. 70. 7.7 0.3 O099201700025 70. 80. 7.57 0.21 O099201700026 80. 90. 7.24 0.23 O099201700027 ENDDATA 11 0 O099201700028 ENDSUBENT 27 0 O099201799999 SUBENT O0992018 20040321 0000O099201800001 BIB 4 7 O099201800002 REACTION (67-HO-165(PIP,F),,DA,FF,REL) Fig.3 O099201800003 STATUS (CURVE) By CAJAD. O099201800004 COMMENT -By authors. The differential angular cross sections O099201800005 for fission fragments were obtained by using muscovite O099201800006 mica track detectors. O099201800007 ERR-ANALYS (DATA-ERR) The uncertainty is shown on figures, withoutO099201800008 any analysis. O099201800009 ENDBIB 7 0 O099201800010 COMMON 1 3 O099201800011 EN O099201800012 MEV O099201800013 80. O099201800014 ENDCOMMON 3 0 O099201800015 DATA 4 9 O099201800016 ANG-MIN ANG-MAX DATA DATA-ERR O099201800017 ADEG ADEG ARB-UNITS ARB-UNITS O099201800018 0. 10. 4.89 0.25 O099201800019 10. 20. 4.78 0.27 O099201800020 20. 30. 4.6 0.3 O099201800021 30. 40. 4.64 0.21 O099201800022 40. 50. 4.53 0.17 O099201800023 50. 60. 4.32 0.27 O099201800024 60. 70. 4.08 0.15 O099201800025 70. 80. 3.92 0.23 O099201800026 80. 90. 3.5 0.21 O099201800027 ENDDATA 11 0 O099201800028 ENDSUBENT 27 0 O099201899999 SUBENT O0992019 20040321 0000O099201900001 BIB 4 7 O099201900002 REACTION (92-U-0(PIP,F)MASS,,PY) Fig.4 O099201900003 STATUS (CURVE) By CAJAD. O099201900004 COMMENT -By authors. The mass distribution were obtained by O099201900005 using a phosphate glass track detector. O099201900006 ERR-ANALYS (DATA-ERR) The uncertainty is shown on figure without O099201900007 any analysis. O099201900008 (ERR-DIG) Data-point reader uncertainty. O099201900009 ENDBIB 7 0 O099201900010 COMMON 2 3 O099201900011 EN ERR-DIG O099201900012 MEV PER-CENT O099201900013 80. 3. O099201900014 ENDCOMMON 3 0 O099201900015 DATA 3 10 O099201900016 MASS DATA DATA-ERR O099201900017 NO-DIM PC/REAC PER-CENT O099201900018 73. 0.62 29. O099201900019 80. 1.15 17. O099201900020 87. 2.21 O099201900021 103. 5.8 16. O099201900022 112. 6. O099201900023 119. 6.2 18. O099201900024 128. 5.2 O099201900025 139. 2.8 21. O099201900026 145. 1.63 O099201900027 153. 0.75 25. O099201900028 ENDDATA 12 0 O099201900029 ENDSUBENT 28 0 O099201999999 SUBENT O0992020 20040321 0000O099202000001 BIB 4 5 O099202000002 REACTION (92-U-0(PIN,F)MASS,,PY) O099202000003 STATUS (CURVE) By CAJAD. O099202000004 COMMENT -By authors. The mass distribution was obtained by O099202000005 using a soda lime glass track detector. O099202000006 ERR-ANALYS (ERR-DIG) Data-point reader uncertainty. O099202000007 ENDBIB 5 0 O099202000008 COMMON 2 3 O099202000009 EN ERR-DIG O099202000010 MEV PER-CENT O099202000011 80. 3. O099202000012 ENDCOMMON 3 0 O099202000013 DATA 2 9 O099202000014 MASS DATA O099202000015 NO-DIM PC/REAC O099202000016 83. 2.16 O099202000017 89. 3.37 O099202000018 95. 4.57 O099202000019 106. 4.9 O099202000020 118. 5.64 O099202000021 128. 5.84 O099202000022 140. 5.26 O099202000023 144. 3. O099202000024 148. 1.63 O099202000025 ENDDATA 11 0 O099202000026 ENDSUBENT 25 0 O099202099999 ENDENTRY 20 0 O099299999999