ENTRY E1851 20040311 0000E185100000001 SUBENT E1851001 20040311 0000E185100100001 BIB 12 55 E185100100002 TITLE Characteristics of binary scission configurations in E185100100003 proton-induced fission of actinides E185100100004 AUTHOR (Y.L.Zhao, T.Ohtsuki, Y.Nagame, I.Nishinaka, E185100100005 K.Tsukada, S.Ichikawa, H.Ikezoe, Y.Hatsukawa, K.Hata, E185100100006 M.Tanikawa, Z.Qin, K.Sueki, Y.Oura, H.Kudo, E185100100007 H.Nakahara) E185100100008 INSTITUTE (2JPNTMU)Department of Chemistry E185100100009 (2JPNTOH)Laboratory of Nuclear Science E185100100010 (2JPNJAE) E185100100011 (2JPNTOK)Department of Chemistry E185100100012 (2JPNNII)Department of Chemistry E185100100013 REFERENCE (J,JRN,239,(1),113,1999) E185100100014 REL-REF (N,,Y.Nagame+,J,PL/B,387,26,1996) E185100100015 Detail of experimental procedure and two-Gaussian E185100100016 analysis E185100100017 (N,,Y.Nagame+,J,JRN,239,97,1999) E185100100018 PART-DET (FF) E185100100019 SAMPLE - Chemical-form of target is element. E185100100020 - Physical-form of target is solid. E185100100021 METHOD (TOF)Flight pathes of two telescopes are 55 cm and 50 E185100100022 cm, respectively. E185100100023 FACILITY (VDGT,2JPNJAE) E185100100024 DETECTOR Solid angle: 0.17 and 32 msr for ToF1 and ToF2, E185100100025 respectively E185100100026 Detector resolution is about 2.5MeV.(Overall E185100100027 resolution of kinetic energy. Resolution of mass is E185100100028 about 2.0 u.) E185100100029 Calibration: Velocity calibration was performed using E185100100030 the 240 MeV 127I beam to bombard the thin targets (60 E185100100031 micro-gram/cm2 thick), natAg, natIn, and 209Bi. Each E185100100032 target was evaporated on 30 micro-gram/cm2 thick E185100100033 carbon foils. The recoil nuclei and the elastically E185100100034 scattered 127I ions were detected with the present ToF E185100100035 system. E185100100036 (MCPLT)Used as stop detector of ToF1 telescope placed E185100100037 at theta(lab)=50 deg E185100100038 (SIBAR)Used as stop and energy signals, located behind E185100100039 the ToF1 stop detector E185100100040 (MCPLT)Used as start detector of ToF2 telescope placed E185100100041 at theta(lab)=130 deg E185100100042 (PPAC)Used as stop detector of ToF2 telescope placed E185100100043 at theta(lab)=130 deg E185100100044 ADD-RES Distance of two charge centers at scission E185100100045 configurations evaluated from the total kinetic energy E185100100046 of the fragment mass for 13 MeV p+238U fission. See E185100100047 Fig.2 of this reference. E185100100048 (COMP)Two-gaussian analysis. The elongation properties E185100100049 of nuclei at scission in a wide range of E185100100050 actinides fissions are studied. The results E185100100051 suggest that the compact and the elongated E185100100052 scission configurations in light actinides E185100100053 fission smoothly change to the scission E185100100054 properties of the symmetric and the asymetric E185100100055 modes in heavy actinides fission. E185100100056 HISTORY (20031104T)Data converted from EXFOR O0699 E185100100057 ENDBIB 55 0 E185100100058 NOCOMMON 0 0 E185100100059 ENDSUBENT 58 0 E185100199999 SUBENT E1851002 20040311 0000E185100200001 BIB 6 16 E185100200002 REACTION (92-U-238(P,F)MASS,PRE,FY/DE,,REL) E185100200003 DATA: Unit is Counts. E185100200004 EN-SEC (E,FF)Total kinetic energy (TKE) for fission fragments E185100200005 MISC-COL (MISC1)Mass yield corresponding to low-total kinetic E185100200006 energy component, given in Counts E185100200007 (MISC2)Mass yield corresponding to high-total kinetic E185100200008 energy component, given in Counts E185100200009 SAMPLE - Target-thickness is about 0.07 mg/cm**2. E185100200010 - Backing is carbon. E185100200011 - Backing-thickness is 0.03 mg/cm**2. E185100200012 ANALYSIS Decomposition of total kinetic energy (TKE) E185100200013 distribution into low- and high-TKE components was E185100200014 done by using the two-Gaussian analysis, described in E185100200015 detail in [Y.Nagame et al., Phys. Lett. B387(1996)26]. E185100200016 STATUS (TABLE)Data (Fig.1, p114 in reference) received from E185100200017 Y.L.Zhao (1999.11.17) E185100200018 ENDBIB 16 0 E185100200019 COMMON 2 3 E185100200020 EN MASS E185100200021 MEV NO-DIM E185100200022 13.0 126.0 E185100200023 ENDCOMMON 3 0 E185100200024 DATA 4 33 E185100200025 E DATA MISC1 MISC2 E185100200026 MEV ARB-UNITS ARB-UNITS ARB-UNITS E185100200027 132.0 0.98636 1.6148 E185100200028 134.0 1.973 2.6463 E185100200029 136.0 2.9597 4.2002 E185100200030 138.0 9.8675 6.4563 E185100200031 140.0 6.9078 9.6118 E185100200032 142.0 16.777 13.859 E185100200033 144.0 22.701 19.352 E185100200034 146.0 21.715 26.172 0.15012 E185100200035 148.0 28.628 34.28 0.26943 E185100200036 150.0 39.49 43.485 0.46682 E185100200037 152.0 44.43 53.424 0.78079 E185100200038 154.0 60.27 63.567 1.2607 E185100200039 156.0 69.25 73.253 1.965 E185100200040 158.0 82.757 81.755 2.9566 E185100200041 160.0 98.962 88.369 4.2945 E185100200042 162.0 114.58 92.508 6.0216 E185100200043 164.0 117.55 93.79 8.1508 E185100200044 166.0 83.968 92.095 10.651 E185100200045 168.0 102.75 87.58 13.435 E185100200046 170.0 110.66 80.663 16.36 E185100200047 172.0 95.963 71.951 19.231 E185100200048 174.0 74.98 62.159 21.822 E185100200049 176.0 68.186 52.007 23.905 E185100200050 178.0 69.178 42.142 25.28 E185100200051 180.0 64.241 33.073 25.807 E185100200052 182.0 56.338 25.137 25.432 E185100200053 184.0 52.389 18.504 24.194 E185100200054 186.0 26.69 13.192 22.218 E185100200055 188.0 26.692 9.1085 19.697 E185100200056 190.0 16.807 6.0909 16.857 E185100200057 192.0 11.864 3.9447 13.927 E185100200058 194.0 9.8873 2.4743 11.107 E185100200059 196.0 4.944 1.503 8.5513 E185100200060 ENDDATA 35 0 E185100200061 ENDSUBENT 60 0 E185100299999 SUBENT E1851003 20040311 0000E185100300001 BIB 6 16 E185100300002 REACTION (92-U-238(P,F)MASS,PRE,FY/DE,,REL) E185100300003 DATA: Unit is Counts. E185100300004 EN-SEC (E,FF)Total kinetic energy (TKE) for fission fragments E185100300005 MISC-COL (MISC1)Mass yield corresponding to low-total kinetic E185100300006 energy component, given in Counts E185100300007 (MISC2)Mass yield corresponding to high-total kinetic E185100300008 energy component, given in Counts E185100300009 SAMPLE - Target-thickness is about 0.07 mg/cm**2. E185100300010 - Backing is carbon. E185100300011 - Backing-thickness is 0.03 mg/cm**2. E185100300012 ANALYSIS Decomposition of total kinetic energy (TKE) E185100300013 distribution into low- and high-TKE components was E185100300014 done by using the two-Gaussian analysis, described in E185100300015 detail in [Y.Nagame et al., Phys. Lett. B387(1996)26]. E185100300016 STATUS (TABLE)Data (Fig.1, p114 in reference) received from E185100300017 Y.L.Zhao (1999.11.17) E185100300018 ENDBIB 16 0 E185100300019 COMMON 2 3 E185100300020 EN MASS E185100300021 MEV NO-DIM E185100300022 13.0 128.0 E185100300023 ENDCOMMON 3 0 E185100300024 DATA 4 35 E185100300025 E DATA MISC1 MISC2 E185100300026 MEV ARB-UNITS ARB-UNITS ARB-UNITS E185100300027 136.0 8.8776 4.5688 0.01147 E185100300028 138.0 9.8648 7.0204 0.02469 E185100300029 140.0 8.8797 10.446 0.05129 E185100300030 142.0 12.827 15.053 0.10281 E185100300031 144.0 22.695 21.006 0.19889 E185100300032 146.0 27.633 28.386 0.37127 E185100300033 148.0 33.557 37.147 0.66877 E185100300034 150.0 33.559 47.075 1.1624 E185100300035 152.0 51.329 57.771 1.9497 E185100300036 154.0 47.385 68.656 3.1557 E185100300037 156.0 85.008 79.013 4.9285 E185100300038 158.0 89.9 88.059 7.4276 E185100300039 160.0 112.57 95.039 10.802 E185100300040 162.0 118.5 99.33 15.158 E185100300041 164.0 108.63 100.53 20.527 E185100300042 166.0 130.3 98.536 26.822 E185100300043 168.0 147.3 93.525 33.82 E185100300044 170.0 150.98 85.964 41.15 E185100300045 172.0 152.13 76.516 48.315 E185100300046 174.0 135.35 65.954 54.738 E185100300047 176.0 128.44 55.053 59.844 E185100300048 178.0 112.64 44.502 63.133 E185100300049 180.0 96.837 34.836 64.268 E185100300050 182.0 65.222 26.407 63.133 E185100300051 184.0 61.272 19.385 59.844 E185100300052 186.0 72.149 13.781 54.738 E185100300053 188.0 59.303 9.4869 48.315 E185100300054 190.0 38.55 6.3245 41.15 E185100300055 192.0 30.644 4.0831 33.82 E185100300056 194.0 19.771 2.5527 26.822 E185100300057 196.0 21.75 1.5454 20.527 E185100300058 198.0 12.853 0.90608 15.158 E185100300059 200.0 11.865 0.51444 10.802 E185100300060 202.0 3.955 0.28284 7.4276 E185100300061 204.0 4.944 0.1506 4.9285 E185100300062 ENDDATA 37 0 E185100300063 ENDSUBENT 62 0 E185100399999 SUBENT E1851004 20040311 0000E185100400001 BIB 6 16 E185100400002 REACTION (92-U-238(P,F)MASS,PRE,FY/DE,,REL) E185100400003 DATA: Unit is Counts. E185100400004 EN-SEC (E,FF)Total kinetic energy (TKE) for fission fragments E185100400005 MISC-COL (MISC1)Mass yield corresponding to low-total kinetic E185100400006 energy component, given in Counts E185100400007 (MISC2)Mass yield corresponding to high-total kinetic E185100400008 energy component, given in Counts E185100400009 SAMPLE - Target-thickness is about 0.07 mg/cm**2. E185100400010 - Backing is carbon. E185100400011 - Backing-thickness is 0.03 mg/cm**2. E185100400012 ANALYSIS Decomposition of total kinetic energy (TKE) E185100400013 distribution into low- and high-TKE components was E185100400014 done by using the two-Gaussian analysis, described in E185100400015 detail in [Y.Nagame et al., Phys. Lett. B387(1996)26]. E185100400016 STATUS (TABLE)Data (Fig.1, p114 in reference) received from E185100400017 Y.L.Zhao (1999.11.17) E185100400018 ENDBIB 16 0 E185100400019 COMMON 2 3 E185100400020 EN MASS E185100400021 MEV NO-DIM E185100400022 13.0 130.0 E185100400023 ENDCOMMON 3 0 E185100400024 DATA 4 44 E185100400025 E DATA MISC1 MISC2 E185100400026 MEV ARB-UNITS ARB-UNITS ARB-UNITS E185100400027 124.0 0.98547 0.17658 0.00017 E185100400028 126.0 0.98573 0.32857 0.00044 E185100400029 128.0 1.9716 0.59203 0.00114 E185100400030 130.0 0.98581 1.0329 0.0028 E185100400031 132.0 0.98586 1.7452 0.00668 E185100400032 134.0 1.972 2.8551 0.01533 E185100400033 136.0 4.9308 4.5232 0.03397 E185100400034 138.0 4.9313 6.9388 0.07259 E185100400035 140.0 7.8908 10.308 0.14962 E185100400036 142.0 11.837 14.827 0.29748 E185100400037 144.0 15.785 20.653 0.57049 E185100400038 146.0 19.732 27.857 1.0553 E185100400039 148.0 29.602 36.383 1.8829 E185100400040 150.0 48.354 46.016 3.2405 E185100400041 152.0 54.279 56.356 5.3795 E185100400042 154.0 65.141 66.834 8.6138 E185100400043 156.0 84.887 76.751 13.304 E185100400044 158.0 94.766 85.348 19.82 E185100400045 160.0 118.47 91.903 28.481 E185100400046 162.0 146.12 95.829 39.477 E185100400047 164.0 149.09 96.758 52.779 E185100400048 166.0 178.73 94.604 68.064 E185100400049 168.0 205.41 89.568 84.665 E185100400050 170.0 194.56 82.116 101.58 E185100400051 172.0 194.57 72.9 117.56 E185100400052 174.0 197.55 62.669 131.24 E185100400053 176.0 205.46 52.168 141.31 E185100400054 178.0 184.61 42.052 146.77 E185100400055 180.0 173.01 32.824 147.03 E185100400056 182.0 168.95 24.81 142.08 E185100400057 184.0 148.21 18.159 132.43 E185100400058 186.0 134.39 12.87 119.06 E185100400059 188.0 94.866 8.8325 103.25 E185100400060 190.0 73.13 5.8698 86.361 E185100400061 192.0 72.147 3.7774 69.679 E185100400062 194.0 57.326 2.3539 54.227 E185100400063 196.0 39.537 1.4204 40.706 E185100400064 198.0 44.482 0.82996 29.474 E185100400065 200.0 20.759 0.46961 20.585 E185100400066 202.0 9.8858 0.2573 13.868 E185100400067 204.0 8.8977 0.13651 9.0111 E185100400068 206.0 5.9324 0.07013 5.6479 E185100400069 208.0 2.9663 0.03489 3.4145 E185100400070 210.0 1.9775 0.01681 1.9912 E185100400071 ENDDATA 46 0 E185100400072 ENDSUBENT 71 0 E185100499999 SUBENT E1851005 20040311 0000E185100500001 BIB 6 16 E185100500002 REACTION (92-U-238(P,F)MASS,PRE,FY/DE,,REL) E185100500003 DATA: Unit is Counts. E185100500004 EN-SEC (E,FF)Total kinetic energy (TKE) for fission fragments E185100500005 MISC-COL (MISC1)Mass yield corresponding to low-total kinetic E185100500006 energy component, given in Counts E185100500007 (MISC2)Mass yield corresponding to high-total kinetic E185100500008 energy component, given in Counts E185100500009 SAMPLE - Target-thickness is about 0.07 mg/cm**2. E185100500010 - Backing is carbon. E185100500011 - Backing-thickness is 0.03 mg/cm**2. E185100500012 ANALYSIS Decomposition of total kinetic energy (TKE) E185100500013 distribution into low- and high-TKE components was E185100500014 done by using the two-Gaussian analysis, described in E185100500015 detail in [Y.Nagame et al., Phys. Lett. B387(1996)26]. E185100500016 STATUS (TABLE)Data (Fig.1, p114 in reference) received from E185100500017 Y.L.Zhao (1999.11.17) E185100500018 ENDBIB 16 0 E185100500019 COMMON 2 3 E185100500020 EN MASS E185100500021 MEV NO-DIM E185100500022 13.0 132.0 E185100500023 ENDCOMMON 3 0 E185100500024 DATA 4 40 E185100500025 E DATA MISC1 MISC2 E185100500026 MEV ARB-UNITS ARB-UNITS ARB-UNITS E185100500027 134.0 4.929 2.1326 0.0348 E185100500028 136.0 3.9437 3.3732 0.07627 E185100500029 138.0 9.8602 5.1662 0.16114 E185100500030 140.0 10.848 7.6612 0.32827 E185100500031 142.0 15.779 11.001 0.64477 E185100500032 144.0 19.727 15.295 1.221 E185100500033 146.0 23.675 20.592 2.2295 E185100500034 148.0 24.663 26.843 3.925 E185100500035 150.0 44.397 33.882 6.6622 E185100500036 152.0 66.107 41.41 10.903 E185100500037 154.0 74.006 49.006 17.205 E185100500038 156.0 81.908 56.155 26.175 E185100500039 158.0 120.4 62.307 38.396 E185100500040 160.0 136.21 66.939 54.304 E185100500041 162.0 158.92 69.635 74.051 E185100500042 164.0 178.68 70.142 97.361 E185100500043 166.0 183.63 68.412 123.42 E185100500044 168.0 199.17 64.607 150.85 E185100500045 170.0 206.37 59.08 177.77 E185100500046 172.0 219.22 52.311 201.99 E185100500047 174.0 256.76 44.849 221.28 E185100500048 176.0 282.45 37.232 233.73 E185100500049 178.0 260.75 29.928 238.03 E185100500050 180.0 244.96 23.294 233.73 E185100500051 182.0 247.94 17.555 221.28 E185100500052 184.0 216.34 12.811 201.99 E185100500053 186.0 190.67 9.0519 177.77 E185100500054 188.0 173.89 6.1931 150.85 E185100500055 190.0 165.99 4.1028 123.42 E185100500056 192.0 126.48 2.6318 97.361 E185100500057 194.0 97.83 1.6347 74.051 E185100500058 196.0 63.247 0.98313 54.304 E185100500059 198.0 48.426 0.57252 38.396 E185100500060 200.0 36.569 0.32283 26.175 E185100500061 202.0 27.676 0.17626 17.205 E185100500062 204.0 14.827 0.09318 10.903 E185100500063 206.0 7.908 0.0477 6.6622 E185100500064 208.0 6.9201 0.02364 3.925 E185100500065 210.0 1.9773 0.01135 2.2295 E185100500066 212.0 0.98873 0.00527 1.221 E185100500067 ENDDATA 42 0 E185100500068 ENDSUBENT 67 0 E185100599999 SUBENT E1851006 20040311 0000E185100600001 BIB 6 16 E185100600002 REACTION (90-TH-232(P,F)MASS,PRE,FY,,REL) E185100600003 MISC-COL (MISC1)Mass yield corresponding to low-total kinetic E185100600004 energy component, given in Counts E185100600005 (MISC2)Mass yield corresponding to high-total kinetic E185100600006 energy component, given in Counts E185100600007 SAMPLE - Target-thickness is about 0.07 mg/cm**2. E185100600008 - Backing is carbon. E185100600009 - Backing-thickness is 0.03 mg/cm**2. E185100600010 ANALYSIS Two different methods are used for estimating the E185100600011 width of distribution: (1) Integration method which is E185100600012 done by sorting program called Lisa, (2)Standard E185100600013 deviation which was obtained using the conventional E185100600014 formula of the deviation theory. E185100600015 FLAG (1.) Standard deviation method was used. E185100600016 STATUS (TABLE)Data (Fig.2a, p115 in reference) received from E185100600017 Y.L.Zhao (1999.11.17) E185100600018 ENDBIB 16 0 E185100600019 COMMON 1 3 E185100600020 EN E185100600021 MEV E185100600022 13.0 E185100600023 ENDCOMMON 3 0 E185100600024 DATA 5 54 E185100600025 MASS DATA MISC1 MISC2 FLAG E185100600026 NO-DIM ARB-UNITS ARB-UNITS ARB-UNITS NO-DIM E185100600027 116.0 0.28428 E185100600028 117.0 0.28727 E185100600029 118.0 0.2988 E185100600030 119.0 0.29826 E185100600031 120.0 0.28843 E185100600032 121.0 0.28037 E185100600033 122.0 0.26979 E185100600034 123.0 0.2866 E185100600035 124.0 0.27376 E185100600036 124.0 0.27341 0.24823 0.025176 1.0 E185100600037 125.0 0.27325 E185100600038 126.0 0.3222 E185100600039 126.0 0.32343 0.23349 0.089942 1.0 E185100600040 127.0 0.3247 E185100600041 128.0 0.36788 E185100600042 128.0 0.39823 0.20148 0.19675 1.0 E185100600043 129.0 0.42861 E185100600044 130.0 0.52325 E185100600045 130.0 0.56361 0.17747 0.38614 1.0 E185100600046 131.0 0.60406 E185100600047 132.0 0.68133 E185100600048 132.0 0.72872 0.12145 0.60726 1.0 E185100600049 133.0 0.77613 E185100600050 134.0 0.85208 E185100600051 134.0 0.87837 0.09786 0.78049 1.0 E185100600052 135.0 0.90467 E185100600053 136.0 0.95924 E185100600054 137.0 0.95007 E185100600055 138.0 0.97901 E185100600056 139.0 0.99992 E185100600057 140.0 1.0 E185100600058 141.0 0.93039 E185100600059 142.0 0.90292 E185100600060 143.0 0.80075 E185100600061 144.0 0.746 E185100600062 145.0 0.64013 E185100600063 146.0 0.52555 E185100600064 147.0 0.4175 E185100600065 148.0 0.33505 E185100600066 149.0 0.23858 E185100600067 150.0 0.19749 E185100600068 151.0 0.12463 E185100600069 152.0 0.095328 E185100600070 153.0 0.06604 E185100600071 154.0 0.044518 E185100600072 155.0 0.031255 E185100600073 156.0 0.016499 E185100600074 157.0 0.0077467 E185100600075 158.0 0.004747 E185100600076 159.0 0.0037472 E185100600077 160.0 0.0017474 E185100600078 161.0 0.0014977 E185100600079 162.0 0.00024949 E185100600080 163.0 0.0012475 E185100600081 ENDDATA 56 0 E185100600082 ENDSUBENT 81 0 E185100699999 SUBENT E1851007 20040311 0000E185100700001 BIB 6 16 E185100700002 REACTION (92-U-238(P,F)MASS,PRE,FY,,REL) E185100700003 MISC-COL (MISC1)Mass yield corresponding to low-total kinetic E185100700004 energy component, given in Counts E185100700005 (MISC2)Mass yield corresponding to high-total kinetic E185100700006 energy component, given in Counts E185100700007 SAMPLE - Target-thickness is about 0.07 mg/cm**2. E185100700008 - Backing is carbon. E185100700009 - Backing-thickness is 0.03 mg/cm**2. E185100700010 ANALYSIS Two different methods are used for estimating the E185100700011 width of distribution: (1) Integration method which is E185100700012 done by sorting program called Lisa, (2)Standard E185100700013 deviation which was obtained using the conventional E185100700014 formula of the deviation theory. E185100700015 FLAG (1.) Standard deviation method was used. E185100700016 STATUS (TABLE)Data (Fig.2b, p115 in reference) received from E185100700017 Y.L.Zhao (1999.11.17) E185100700018 ENDBIB 16 0 E185100700019 COMMON 1 3 E185100700020 EN E185100700021 MEV E185100700022 13.0 E185100700023 ENDCOMMON 3 0 E185100700024 DATA 5 54 E185100700025 MASS DATA MISC1 MISC2 FLAG E185100700026 NO-DIM ARB-UNITS ARB-UNITS ARB-UNITS NO-DIM E185100700027 118.0 0.18494 E185100700028 119.0 0.20723 E185100700029 120.0 0.19897 E185100700030 121.0 0.18626 E185100700031 122.0 0.20613 E185100700032 123.0 0.20407 E185100700033 124.0 0.24383 E185100700034 124.0 0.25402 0.21995 0.03407 1.0 E185100700035 125.0 0.26542 E185100700036 126.0 0.27843 E185100700037 126.0 0.29368 0.23261 0.061072 1.0 E185100700038 127.0 0.30893 E185100700039 128.0 0.38948 E185100700040 128.0 0.42878 0.26691 0.16187 1.0 E185100700041 129.0 0.4697 E185100700042 130.0 0.56704 E185100700043 130.0 0.61411 0.25174 0.36237 1.0 E185100700044 131.0 0.66127 E185100700045 132.0 0.73252 E185100700046 132.0 0.78614 0.18782 0.59833 1.0 E185100700047 133.0 0.83975 E185100700048 133.0 0.91672 0.12946 0.78726 1.0 E185100700049 134.0 0.87634 E185100700050 135.0 0.9571 E185100700051 136.0 0.96589 E185100700052 137.0 0.97981 E185100700053 138.0 0.9912 E185100700054 139.0 1.0 E185100700055 140.0 0.99687 E185100700056 141.0 0.90733 E185100700057 142.0 0.87056 E185100700058 143.0 0.84372 E185100700059 144.0 0.7885 E185100700060 145.0 0.67956 E185100700061 146.0 0.62847 E185100700062 147.0 0.56714 E185100700063 148.0 0.4658 E185100700064 149.0 0.37512 E185100700065 150.0 0.33608 E185100700066 151.0 0.29124 E185100700067 152.0 0.22693 E185100700068 153.0 0.18247 E185100700069 154.0 0.14622 E185100700070 155.0 0.11033 E185100700071 156.0 0.088797 E185100700072 157.0 0.061119 E185100700073 158.0 0.040965 E185100700074 159.0 0.033113 E185100700075 160.0 0.019108 E185100700076 161.0 0.016035 E185100700077 162.0 0.0098883 E185100700078 163.0 0.0037501 E185100700079 164.0 0.0040906 E185100700080 165.0 0.0037484 E185100700081 ENDDATA 56 0 E185100700082 ENDSUBENT 81 0 E185100799999 SUBENT E1851008 20040311 0000E185100800001 BIB 6 16 E185100800002 REACTION (94-PU-244(P,F)MASS,PRE,FY,,REL) E185100800003 MISC-COL (MISC1)Mass yield corresponding to low-total kinetic E185100800004 energy component, given in Counts E185100800005 (MISC2)Mass yield corresponding to high-total kinetic E185100800006 energy component, given in Counts E185100800007 SAMPLE - Target-thickness is 0.06 mg/cm**2. E185100800008 - Backing: Electrodeposited onto Ni foil E185100800009 - Backing-thickness: 0.1 micro-meter E185100800010 ANALYSIS Two different methods are used for estimating the E185100800011 width of distribution: (1) Integration method which is E185100800012 done by sorting program called Lisa, (2)Standard E185100800013 deviation which was obtained using the conventional E185100800014 formula of the deviation theory. E185100800015 FLAG (1.) Standard deviation method was used. E185100800016 STATUS (TABLE)Data (Fig.2c, p115 in reference) received from E185100800017 Y.L.Zhao (1999.11.17) E185100800018 ENDBIB 16 0 E185100800019 COMMON 1 3 E185100800020 EN E185100800021 MEV E185100800022 15.0 E185100800023 ENDCOMMON 3 0 E185100800024 DATA 5 63 E185100800025 MASS DATA MISC1 MISC2 FLAG E185100800026 NO-DIM ARB-UNITS ARB-UNITS ARB-UNITS NO-DIM E185100800027 122.0 0.34601 E185100800028 123.0 0.36858 E185100800029 124.0 0.35919 E185100800030 124.0 0.36721 0.34977 0.017438 1.0 E185100800031 125.0 0.37523 E185100800032 126.0 0.39725 E185100800033 126.0 0.41559 0.33723 0.078362 1.0 E185100800034 127.0 0.43395 E185100800035 128.0 0.48015 E185100800036 128.0 0.50802 0.2943 0.21372 1.0 E185100800037 129.0 0.5359 E185100800038 130.0 0.58859 E185100800039 130.0 0.62475 0.27799 0.34676 1.0 E185100800040 131.0 0.6609 E185100800041 132.0 0.70742 E185100800042 132.0 0.73465 0.19074 0.54391 1.0 E185100800043 133.0 0.76188 E185100800044 134.0 0.83801 E185100800045 134.0 0.86088 0.064285 0.79659 1.0 E185100800046 135.0 0.88376 E185100800047 136.0 0.92566 E185100800048 137.0 0.98054 E185100800049 138.0 1.0 E185100800050 139.0 0.98453 E185100800051 140.0 0.96659 E185100800052 141.0 0.96203 E185100800053 142.0 0.9036 E185100800054 143.0 0.88847 E185100800055 144.0 0.84994 E185100800056 145.0 0.79628 E185100800057 146.0 0.75124 E185100800058 147.0 0.68773 E185100800059 148.0 0.62248 E185100800060 149.0 0.55744 E185100800061 150.0 0.53147 E185100800062 151.0 0.47085 E185100800063 152.0 0.41868 E185100800064 153.0 0.37536 E185100800065 154.0 0.32076 E185100800066 155.0 0.28817 E185100800067 156.0 0.24241 E185100800068 157.0 0.21126 E185100800069 158.0 0.17449 E185100800070 159.0 0.146 E185100800071 160.0 0.12208 E185100800072 161.0 0.10291 E185100800073 162.0 0.081115 E185100800074 163.0 0.072489 E185100800075 164.0 0.055101 E185100800076 165.0 0.03895 E185100800077 166.0 0.027361 E185100800078 167.0 0.024019 E185100800079 168.0 0.020156 E185100800080 169.0 0.012266 E185100800081 170.0 0.0082324 E185100800082 171.0 0.0049039 E185100800083 172.0 0.0052508 E185100800084 173.0 0.0049 E185100800085 174.0 0.0029737 E185100800086 175.0 0.0013999 E185100800087 176.0 0.001224 E185100800088 177.0 0.0012236 E185100800089 178.0 0.00052454 E185100800090 ENDDATA 65 0 E185100800091 ENDSUBENT 90 0 E185100899999 ENDENTRY 8 0 E185199999999