ENTRY F0930 20080528 F032F093000000001 SUBENT F0930001 20080528 F032F093000100001 BIB 8 10 F093000100002 TITLE A study of (7/2)- isobaric analogue resonances in odd F093000100003 isotopes of Sb. F093000100004 AUTHOR (R.Arking,R.N.Boyd,J.C.Lombardi,A.B.Robbins,B.Gonsior) F093000100005 INSTITUTE (2GERKLN,1USARUT) F093000100006 REFERENCE (J,NP/A,155,480,1970) F093000100007 FACILITY (VDGT,1USARUT) F093000100008 SAMPLE Isotopically enriched targets of 124Sn, 122Sn and 120SnF093000100009 were used. F093000100010 ERR-ANALYS (ERR-DIG) Data digitizing error F093000100011 HISTORY (20080423C) F093000100012 ENDBIB 10 0 F093000100013 NOCOMMON 0 0 F093000100014 ENDSUBENT 13 0 F093000199999 SUBENT F0930002 20080528 F032F093000200001 BIB 5 12 F093000200002 REACTION (50-SN-120(P,EL)50-SN-120,,DA,,RTH) F093000200003 DETECTOR (SILI) 2 mm Si(Li) detectors. F093000200004 (SIBAR) 2 mm surface-barrier detectors. Each detector F093000200005 was mounted with a collimator and anti-scattering F093000200006 baffle on a plate which could be rotated. The angular F093000200007 acceptance was +-1.1 degr. F093000200008 SAMPLE Targets with approximately 300 mu-g/cm2 of tin on 10 F093000200009 mu-g/cm2 of carbon backing were used. F093000200010 ERR-ANALYS The uncertainty in the absolute cross section was F093000200011 estimated to be 5% F093000200012 (ANG-ERR-D) Angle digitizing error F093000200013 STATUS (CURVE)Fig.1 F093000200014 ENDBIB 12 0 F093000200015 COMMON 3 3 F093000200016 EN ANG-ERR-D ERR-DIG F093000200017 MEV ADEG NO-DIM F093000200018 9.85 0.126 0.0007 F093000200019 ENDCOMMON 3 0 F093000200020 DATA 2 29 F093000200021 ANG-CM DATA-CM F093000200022 ADEG NO-DIM F093000200023 25.779 1.0699 F093000200024 30.113 1.0254 F093000200025 35.893 0.98101 F093000200026 40.801 0.88072 F093000200027 45.711 0.80191 F093000200028 50.045 0.74889 F093000200029 55.252 0.77181 F093000200030 60.171 0.79615 F093000200031 65.958 0.83482 F093000200032 70.586 0.84484 F093000200033 75.5 0.80901 F093000200034 80.7 0.74596 F093000200035 85.031 0.66716 F093000200036 90.23 0.58405 F093000200037 95.141 0.51384 F093000200038 100.34 0.48088 F093000200039 105.26 0.47084 F093000200040 109.89 0.48659 F093000200041 115.39 0.51667 F093000200042 120.3 0.55247 F093000200043 125.8 0.58828 F093000200044 130.72 0.61262 F093000200045 135.35 0.62694 F093000200046 140.84 0.62836 F093000200047 145.76 0.61259 F093000200048 150.96 0.60685 F093000200049 155.88 0.59108 F093000200050 160.79 0.56242 F093000200051 165.13 0.54378 F093000200052 ENDDATA 31 0 F093000200053 ENDSUBENT 52 0 F093000299999 SUBENT F0930003 20080528 F032F093000300001 BIB 6 16 F093000300002 REACTION (50-SN-120(P,EL)50-SN-120,,DA) F093000300003 MONITOR The absolute cross sections were obtained by F093000300004 determining the target thickness from 4 MeV cross F093000300005 section data at forward angles where Rutherford F093000300006 scattering predominates. F093000300007 DETECTOR (SILI) 2 mm Si(Li) detectors. F093000300008 (SIBAR) 2 mm surface-barrier detectors. Each detector F093000300009 was mounted with a collimator and anti-scattering F093000300010 baffle on a plate which could be rotated. The angular F093000300011 acceptance was +-1.1 degr. F093000300012 SAMPLE Targets with approximately 300 mu-g/cm2 of tin on 10 F093000300013 mu-g/cm2 of carbon backing were used. F093000300014 ERR-ANALYS The uncertainty in the absolute cross section was F093000300015 estimated to be 5% F093000300016 (EN-ERR-DIG) Energy digitizing error F093000300017 STATUS (CURVE)FIG.2 F093000300018 ENDBIB 16 0 F093000300019 COMMON 3 3 F093000300020 ANG EN-ERR-DIG ERR-DIG F093000300021 ADEG MEV MB/SR F093000300022 165. 0.0002 0.027 F093000300023 ENDCOMMON 3 0 F093000300024 DATA 2 50 F093000300025 EN DATA F093000300026 MEV MB/SR F093000300027 9.9949 19.173 F093000300028 10.006 19.112 F093000300029 10.014 19.113 F093000300030 10.024 19.174 F093000300031 10.034 19.543 F093000300032 10.042 19.604 F093000300033 10.054 19.298 F093000300034 10.062 19.789 F093000300035 10.074 19.789 F093000300036 10.082 20.219 F093000300037 10.091 20.219 F093000300038 10.104 20.22 F093000300039 10.113 20.65 F093000300040 10.131 21.08 F093000300041 10.142 21.878 F093000300042 10.151 21.264 F093000300043 10.162 22.553 F093000300044 10.17 24.271 F093000300045 10.179 24.824 F093000300046 10.191 24.21 F093000300047 10.201 21.327 F093000300048 10.212 18.444 F093000300049 10.222 16.788 F093000300050 10.229 17.831 F093000300051 10.243 19.059 F093000300052 10.252 20.531 F093000300053 10.262 23.415 F093000300054 10.272 22.925 F093000300055 10.281 19.673 F093000300056 10.291 13.723 F093000300057 10.305 10.84 F093000300058 10.312 7.834 F093000300059 10.324 6.3006 F093000300060 10.335 6.3623 F093000300061 10.345 6.608 F093000300062 10.354 7.0992 F093000300063 10.364 7.4062 F093000300064 10.375 7.8974 F093000300065 10.386 8.1431 F093000300066 10.394 8.0821 F093000300067 10.404 8.3891 F093000300068 10.414 8.8802 F093000300069 10.425 9.3714 F093000300070 10.434 9.5558 F093000300071 10.445 9.6788 F093000300072 10.454 9.8631 F093000300073 10.464 10.17 F093000300074 10.474 10.171 F093000300075 10.484 9.9868 F093000300076 10.494 10.662 F093000300077 ENDDATA 52 0 F093000300078 ENDSUBENT 77 0 F093000399999 SUBENT F0930004 20080528 F032F093000400001 BIB 5 9 F093000400002 REACTION (50-SN-120(P,EL)50-SN-120,,POL/DA) F093000400003 SAMPLE Targets with approximately 800 mu-g/cm2 of tin were F093000400004 used. F093000400005 METHOD (DSCAT) Data were taken by the double scattering F093000400006 technique. F093000400007 ERR-ANALYS (EN-ERR-DIG) Energy digitizing error F093000400008 (DATA-ERR) Error bars indicate the relative F093000400009 uncertainty of the measurements F093000400010 STATUS (CURVE)Fig.2 F093000400011 ENDBIB 9 0 F093000400012 COMMON 3 3 F093000400013 ANG EN-ERR-DIG ERR-DIG F093000400014 ADEG MEV NO-DIM F093000400015 135. 0.0007 0.0008 F093000400016 ENDCOMMON 3 0 F093000400017 DATA 3 12 F093000400018 EN DATA DATA-ERR F093000400019 MEV NO-DIM NO-DIM F093000400020 10.018 3.6229E-02 F093000400021 10.059-1.9702E-02 4.1262E-02 F093000400022 10.117 4.4252E-03 F093000400023 10.193 0.17899 F093000400024 10.218 0.19835 F093000400025 10.247 7.6914E-02 F093000400026 10.269 0.24676 F093000400027 10.289 0.37293 F093000400028 10.308 0.4287 F093000400029 10.328 0.33642 F093000400030 10.349 0.11549 F093000400031 10.368 8.3890E-02 F093000400032 ENDDATA 14 0 F093000400033 ENDSUBENT 32 0 F093000499999 SUBENT F0930005 20080528 F032F093000500001 BIB 6 8 F093000500002 REACTION (50-SN-120(P,EL)50-SN-120,,POL/DA,,ANA) F093000500003 INC-SOURCE (POLIS) F093000500004 SAMPLE Targets with approximately 800 mu-g/cm2 of tin were F093000500005 used. F093000500006 METHOD (LRASY)Data were taken with the Rutgers-Ortec polirizedF093000500007 ion source. F093000500008 ERR-ANALYS (EN-ERR-DIG) Energy digitizing error F093000500009 STATUS (CURVE)Fig.2 F093000500010 ENDBIB 8 0 F093000500011 COMMON 3 3 F093000500012 ANG EN-ERR-DIG ERR-DIG F093000500013 ADEG MEV NO-DIM F093000500014 135. 0.0007 0.0008 F093000500015 ENDCOMMON 3 0 F093000500016 DATA 2 6 F093000500017 EN DATA F093000500018 MEV NO-DIM F093000500019 10.159 1.6456E-02 F093000500020 10.238 0.22742 F093000500021 10.248 0.12545 F093000500022 10.258 0.18611 F093000500023 10.276 0.32441 F093000500024 10.296 0.41174 F093000500025 ENDDATA 8 0 F093000500026 ENDSUBENT 25 0 F093000599999 SUBENT F0930006 20080528 F032F093000600001 BIB 6 16 F093000600002 REACTION (50-SN-122(P,EL)50-SN-122,,DA) F093000600003 MONITOR The absolute cross sections were obtained by F093000600004 determining the target thickness from 4 MeV cross F093000600005 section data at forward angles where Rutherford F093000600006 scattering predominates. F093000600007 DETECTOR (SILI) 2 mm Si(Li) detectors. F093000600008 (SIBAR) 2 mm surface-barrier detectors. Each detector F093000600009 was mounted with a collimator and anti-scattering F093000600010 baffle on a plate which could be rotated. The angular F093000600011 acceptance was +-1.1 degr. F093000600012 SAMPLE Targets with approximately 300 mu-g/cm2 of tin on 10 F093000600013 mu-g/cm2 of carbon backing were used. F093000600014 ERR-ANALYS The uncertainty in the absolute cross section was F093000600015 estimated to be 5% F093000600016 (EN-ERR-DIG) Energy digitizing error F093000600017 STATUS (CURVE)Fig.3 F093000600018 ENDBIB 16 0 F093000600019 COMMON 2 3 F093000600020 EN-ERR-DIG ERR-DIG F093000600021 MEV MB/SR F093000600022 0.003 0.050 F093000600023 ENDCOMMON 3 0 F093000600024 DATA 3 165 F093000600025 ANG EN DATA F093000600026 ADEG MEV MB/SR F093000600027 120. 9.9894 32.216 F093000600028 120. 10.012 31.647 F093000600029 120. 10.031 30.319 F093000600030 120. 10.052 30.508 F093000600031 120. 10.073 30.507 F093000600032 120. 10.091 30.127 F093000600033 120. 10.111 30.126 F093000600034 120. 10.132 29.841 F093000600035 120. 10.153 28.702 F093000600036 120. 10.172 27.848 F093000600037 120. 10.193 27.658 F093000600038 120. 10.21 27.847 F093000600039 120. 10.232 27.846 F093000600040 120. 10.251 27.182 F093000600041 120. 10.272 27.276 F093000600042 120. 10.301 28.601 F093000600043 120. 10.311 28.885 F093000600044 120. 10.323 27.937 F093000600045 120. 10.333 27.652 F093000600046 120. 10.341 27.083 F093000600047 120. 10.351 25.945 F093000600048 120. 10.36 24.997 F093000600049 120. 10.37 23.954 F093000600050 120. 10.381 22.342 F093000600051 120. 10.393 22.341 F093000600052 120. 10.401 20.161 F093000600053 120. 10.409 19.876 F093000600054 120. 10.424 19.876 F093000600055 120. 10.43 21.108 F093000600056 120. 10.443 23.192 F093000600057 120. 10.453 25.562 F093000600058 120. 10.461 27.362 F093000600059 120. 10.471 31.533 F093000600060 120. 10.482 32.859 F093000600061 120. 10.492 34.47 F093000600062 120. 10.499 35.702 F093000600063 120. 10.509 35.891 F093000600064 120. 10.518 36.175 F093000600065 120. 10.528 36.27 F093000600066 120. 10.539 35.416 F093000600067 120. 10.553 35.131 F093000600068 120. 10.563 34.657 F093000600069 120. 10.572 34.372 F093000600070 120. 10.583 33.898 F093000600071 120. 10.59 33.613 F093000600072 120. 10.602 32.854 F093000600073 120. 10.612 33.517 F093000600074 120. 10.63 33.043 F093000600075 120. 10.65 32.473 F093000600076 120. 10.67 31.429 F093000600077 120. 10.691 31.618 F093000600078 120. 10.71 31.333 F093000600079 120. 10.73 31.901 F093000600080 120. 10.747 30.573 F093000600081 120. 10.771 30.098 F093000600082 120. 10.79 29.529 F093000600083 140. 9.9965 24.569 F093000600084 140. 10.016 23.901 F093000600085 140. 10.035 23.614 F093000600086 140. 10.055 23.423 F093000600087 140. 10.075 23.707 F093000600088 140. 10.095 23.516 F093000600089 140. 10.116 23.896 F093000600090 140. 10.137 22.847 F093000600091 140. 10.156 21.989 F093000600092 140. 10.176 21.416 F093000600093 140. 10.196 21.796 F093000600094 140. 10.218 21.699 F093000600095 140. 10.235 21.413 F093000600096 140. 10.256 21.412 F093000600097 140. 10.274 22.077 F093000600098 140. 10.316 23.789 F093000600099 140. 10.335 24.455 F093000600100 140. 10.354 23.501 F093000600101 140. 10.376 22.548 F093000600102 140. 10.394 23.499 F093000600103 140. 10.406 23.689 F093000600104 140. 10.417 23.498 F093000600105 140. 10.425 23.783 F093000600106 140. 10.435 23.211 F093000600107 140. 10.445 23.592 F093000600108 140. 10.455 24.544 F093000600109 140. 10.466 24.067 F093000600110 140. 10.473 23.304 F093000600111 140. 10.486 23.304 F093000600112 140. 10.496 22.256 F093000600113 140. 10.505 22.35 F093000600114 140. 10.512 22.159 F093000600115 140. 10.527 22.444 F093000600116 140. 10.534 21.682 F093000600117 140. 10.546 21.872 F093000600118 140. 10.553 20.919 F093000600119 140. 10.564 20.918 F093000600120 140. 10.575 20.727 F093000600121 140. 10.583 20.441 F093000600122 140. 10.595 20.631 F093000600123 140. 10.606 20.249 F093000600124 140. 10.636 19.867 F093000600125 140. 10.656 19.485 F093000600126 140. 10.677 19.484 F093000600127 140. 10.693 19.483 F093000600128 140. 10.713 18.815 F093000600129 140. 10.735 19.576 F093000600130 140. 10.755 18.908 F093000600131 140. 10.777 18.621 F093000600132 140. 10.794 18.049 F093000600133 165. 9.9985 15.379 F093000600134 165. 10.02 16.049 F093000600135 165. 10.04 15.093 F093000600136 165. 10.059 15.381 F093000600137 165. 10.079 15.668 F093000600138 165. 10.098 15.19 F093000600139 165. 10.118 16.147 F093000600140 165. 10.137 15.669 F093000600141 165. 10.158 15.574 F093000600142 165. 10.179 15.957 F093000600143 165. 10.198 15.862 F093000600144 165. 10.217 15.862 F093000600145 165. 10.24 16.149 F093000600146 165. 10.257 16.437 F093000600147 165. 10.277 18.732 F093000600148 165. 10.277 16.533 F093000600149 165. 10.306 20.74 F093000600150 165. 10.308 19.497 F093000600151 165. 10.317 20.167 F093000600152 165. 10.317 21.219 F093000600153 165. 10.33 19.785 F093000600154 165. 10.336 21.506 F093000600155 165. 10.337 20.359 F093000600156 165. 10.348 21.506 F093000600157 165. 10.356 21.793 F093000600158 165. 10.367 22.941 F093000600159 165. 10.377 23.228 F093000600160 165. 10.391 24.28 F093000600161 165. 10.395 25.906 F093000600162 165. 10.396 27.244 F093000600163 165. 10.407 27.244 F093000600164 165. 10.416 28.679 F093000600165 165. 10.427 25.715 F093000600166 165. 10.44 22.847 F093000600167 165. 10.446 19.978 F093000600168 165. 10.456 17.588 F093000600169 165. 10.466 13.668 F093000600170 165. 10.476 10.035 F093000600171 165. 10.49 7.3578 F093000600172 165. 10.498 5.5412 F093000600173 165. 10.508 4.5852 F093000600174 165. 10.518 4.9679 F093000600175 165. 10.529 4.5857 F093000600176 165. 10.543 4.5859 F093000600177 165. 10.56 5.3512 F093000600178 165. 10.568 5.2558 F093000600179 165. 10.578 6.1165 F093000600180 165. 10.589 6.308 F093000600181 165. 10.598 6.5951 F093000600182 165. 10.609 6.7865 F093000600183 165. 10.638 7.4564 F093000600184 165. 10.66 7.4569 F093000600185 165. 10.68 7.4573 F093000600186 165. 10.7 7.7446 F093000600187 165. 10.719 7.5537 F093000600188 165. 10.739 8.6059 F093000600189 165. 10.76 8.5108 F093000600190 165. 10.779 8.798 F093000600191 165. 10.8 8.5116 F093000600192 ENDDATA 167 0 F093000600193 ENDSUBENT 192 0 F093000699999 SUBENT F0930007 20080528 F032F093000700001 BIB 4 7 F093000700002 REACTION (50-SN-122(P,EL)50-SN-122,,POL/DA) F093000700003 SAMPLE Targets with approximately 800 mu-g/cm2 of tin were F093000700004 used. F093000700005 ERR-ANALYS (EN-ERR-DIG) Energy digitizing error F093000700006 (DATA-ERR) Error bars indicate the relative F093000700007 uncertainty of the measurements F093000700008 STATUS (CURVE)Fig.3 F093000700009 ENDBIB 7 0 F093000700010 COMMON 3 3 F093000700011 ANG EN-ERR-DIG ERR-DIG F093000700012 ADEG MEV NO-DIM F093000700013 135. 0.0006 0.001 F093000700014 ENDCOMMON 3 0 F093000700015 DATA 3 14 F093000700016 EN DATA DATA-ERR F093000700017 MEV NO-DIM NO-DIM F093000700018 9.9982-4.8123E-03 4.0637E-02 F093000700019 10.2 2.8518E-02 3.8247E-02 F093000700020 10.298 1.1719E-02 4.0637E-02 F093000700021 10.349-1.2219E-02 4.0637E-02 F093000700022 10.375-1.9408E-02 3.5857E-02 F093000700023 10.397 7.1414E-02 3.5857E-02 F093000700024 10.42 0.12399 4.3028E-02 F093000700025 10.438 0.42756 3.3466E-02 F093000700026 10.458 0.51121 4.5418E-02 F093000700027 10.48 0.54944 3.3466E-02 F093000700028 10.5 0.41318 4.0637E-02 F093000700029 10.549 0.15976 4.7809E-02 F093000700030 10.6 9.9963E-02 5.2590E-02 F093000700031 10.699 3.7744E-02 3.8247E-02 F093000700032 ENDDATA 16 0 F093000700033 ENDSUBENT 32 0 F093000799999 SUBENT F0930008 20080528 F032F093000800001 BIB 6 16 F093000800002 REACTION (50-SN-124(P,EL)50-SN-124,,DA) F093000800003 MONITOR The absolute cross sections were obtained by F093000800004 determining the target thickness from 4 MeV cross F093000800005 section data at forward angles where Rutherford F093000800006 scattering predominates. F093000800007 DETECTOR (SILI) 2 mm Si(Li) detectors. F093000800008 (SIBAR) 2 mm surface-barrier detectors. Each detector F093000800009 was mounted with a collimator and anti-scattering F093000800010 baffle on a plate which could be rotated. The angular F093000800011 acceptance was +-1.1 degr. F093000800012 SAMPLE Targets with approximately 300 mu-g/cm2 of tin on 10 F093000800013 mu-g/cm2 of carbon backing were used. F093000800014 ERR-ANALYS The uncertainty in the absolute cross section was F093000800015 estimated to be 5% F093000800016 (EN-ERR-DIG) Energy digitizing error F093000800017 STATUS (CURVE)Fig.4 F093000800018 ENDBIB 16 0 F093000800019 COMMON 3 3 F093000800020 ANG EN-ERR-DIG ERR-DIG F093000800021 ADEG MEV MB/SR F093000800022 165. 0.0001 0.05 F093000800023 ENDCOMMON 3 0 F093000800024 DATA 2 31 F093000800025 EN DATA F093000800026 MEV MB/SR F093000800027 10.297 16.725 F093000800028 10.32 17.14 F093000800029 10.339 17.036 F093000800030 10.36 17.139 F093000800031 10.379 18.178 F093000800032 10.399 18.282 F093000800033 10.418 18.385 F093000800034 10.438 18.904 F093000800035 10.458 19.32 F093000800036 10.478 20.15 F093000800037 10.499 20.254 F093000800038 10.517 20.981 F093000800039 10.536 22.435 F093000800040 10.56 24.513 F093000800041 10.577 27.318 F093000800042 10.595 31.369 F093000800043 10.617 36.044 F093000800044 10.638 36.771 F093000800045 10.657 23.992 F093000800046 10.675 11.42 F093000800047 10.695 4.5625 F093000800048 10.717 3.2115 F093000800049 10.736 3.1073 F093000800050 10.756 3.2109 F093000800051 10.777 3.8339 F093000800052 10.797 4.4569 F093000800053 10.817 4.5605 F093000800054 10.838 4.8719 F093000800055 10.857 5.2871 F093000800056 10.877 5.9102 F093000800057 10.896 6.1177 F093000800058 ENDDATA 33 0 F093000800059 ENDSUBENT 58 0 F093000899999 SUBENT F0930009 20080528 F032F093000900001 BIB 4 7 F093000900002 REACTION (50-SN-124(P,EL)50-SN-124,,POL/DA) F093000900003 SAMPLE Targets with approximately 800 mu-g/cm2 of tin were F093000900004 used. F093000900005 ERR-ANALYS (EN-ERR-DIG) Energy digitizing error F093000900006 (DATA-ERR) Error bars indicate the relative F093000900007 uncertainty of the measurements F093000900008 STATUS (CURVE)Fig.4 F093000900009 ENDBIB 7 0 F093000900010 COMMON 3 3 F093000900011 ANG EN-ERR-DIG ERR-DIG F093000900012 ADEG MEV NO-DIM F093000900013 135. 0.0007 0.001 F093000900014 ENDCOMMON 3 0 F093000900015 DATA 3 15 F093000900016 EN DATA DATA-ERR F093000900017 MEV NO-DIM NO-DIM F093000900018 10.202 4.2138E-02 4.2105E-02 F093000900019 10.501-3.9247E-02 3.9474E-02 F093000900020 10.576 3.7117E-02 4.4737E-02 F093000900021 10.601 9.7660E-02 4.7368E-02 F093000900022 10.625 0.32399 5.2632E-02 F093000900023 10.652 0.54769 4.4737E-02 F093000900024 10.678 0.62666 5.7895E-02 F093000900025 10.703 0.55825 6.3158E-02 F093000900026 10.728 0.42143 5.5263E-02 F093000900027 10.754 0.3425 5.2632E-02 F093000900028 10.778 0.2162 5.7895E-02 F093000900029 10.803 0.15042 5.0000E-02 F093000900030 10.828 0.14518 5.0000E-02 F093000900031 10.853 0.15309 5.2632E-02 F093000900032 10.905 6.3647E-02 6.3158E-02 F093000900033 ENDDATA 17 0 F093000900034 ENDSUBENT 33 0 F093000999999 SUBENT F0930010 20080528 F032F093001000001 BIB 6 17 F093001000002 REACTION (50-SN-120(P,INL)50-SN-120,PAR,DA) F093001000003 MONITOR The absolute cross sections were obtained by F093001000004 determining the target thickness from 4 MeV cross F093001000005 section data at forward angles where Rutherford F093001000006 scattering predominates. F093001000007 DETECTOR (SILI) 2 mm Si(Li) detectors. F093001000008 (SIBAR) 2 mm surface-barrier detectors. Each detector F093001000009 was mounted with a collimator and anti-scattering F093001000010 baffle on a plate which could be rotated. The angular F093001000011 acceptance was +-1.1 degr. F093001000012 SAMPLE Targets with approximately 300 mu-g/cm2 of tin on 10 F093001000013 mu-g/cm2 of carbon backing were used. F093001000014 ERR-ANALYS The uncertainty in the absolute cross section was F093001000015 estimated to be 5% F093001000016 (EN-ERR-DIG) Energy digitizing error F093001000017 (DATA-ERR) Error from the graphic bars F093001000018 STATUS (CURVE)Fig.5 F093001000019 ENDBIB 17 0 F093001000020 COMMON 2 3 F093001000021 EN-ERR-DIG ERR-DIG F093001000022 MEV MB/SR F093001000023 0.0003 0.0009 F093001000024 ENDCOMMON 3 0 F093001000025 DATA 5 83 F093001000026 E-LVL ANG EN DATA DATA-ERR F093001000027 MEV ADEG MEV MB/SR MB/SR F093001000028 1.18 165. 9.9058 0.22582 F093001000029 1.18 165. 9.9278 0.19736 F093001000030 1.18 165. 9.9499 0.1384 F093001000031 1.18 165. 9.9799 0.14046 F093001000032 1.18 165. 10.006 0.16286 F093001000033 1.18 165. 10.016 0.171 F093001000034 1.18 165. 10.022 0.14864 F093001000035 1.18 165. 10.034 0.24017 F093001000036 1.18 165. 10.038 0.15069 F093001000037 1.18 165. 10.058 0.17104 F093001000038 1.18 165. 10.066 0.21783 F093001000039 1.18 165. 10.072 9.9869E-02 F093001000040 1.18 165. 10.084 0.12022 F093001000041 1.18 165. 10.09 7.7513E-02 F093001000042 1.18 165. 10.114 8.7705E-02 3.4576E-02 F093001000043 1.18 165. 10.144 6.5360E-02 F093001000044 1.18 165. 10.156 9.5880E-02 F093001000045 1.18 165. 10.164 0.12843 F093001000046 1.18 165. 10.172 8.5725E-02 F093001000047 1.18 165. 10.18 0.13658 F093001000048 1.18 165. 10.194 0.10812 F093001000049 1.18 165. 10.2 0.16711 F093001000050 1.18 165. 10.214 0.17932 F093001000051 1.18 165. 10.222 0.15289 F093001000052 1.18 165. 10.234 7.9681E-02 F093001000053 1.18 165. 10.238 6.5447E-02 F093001000054 1.18 165. 10.256 6.9532E-02 F093001000055 1.18 165. 10.262 0.14072 F093001000056 1.18 165. 10.276 0.17735 F093001000057 1.18 165. 10.284 0.26481 F093001000058 1.18 165. 10.298 0.31161 F093001000059 1.18 165. 10.304 0.47025 F093001000060 1.18 165. 10.32 0.49061 F093001000061 1.18 165. 10.332 0.49672 F093001000062 1.18 165. 10.342 0.51707 F093001000063 1.18 165. 10.348 0.41131 F093001000064 1.18 165. 10.354 0.26284 F093001000065 1.18 165. 10.364 0.21607 F093001000066 1.18 165. 10.372 0.17744 F093001000067 1.18 165. 10.384 0.12863 F093001000068 1.18 165. 10.406 0.16526 F093001000069 2.39 125. 9.9018 0.17897 F093001000070 2.39 125. 9.922 0.14402 F093001000071 2.39 125. 9.9563 0.12966 F093001000072 2.39 125. 9.9743 0.18932 F093001000073 2.39 125. 10.002 0.22019 F093001000074 2.39 125. 10.015 0.22432 F093001000075 2.39 125. 10.023 0.24284 F093001000076 2.39 125. 10.039 0.24902 F093001000077 2.39 125. 10.047 0.27371 F093001000078 2.39 125. 10.063 0.26755 F093001000079 2.39 125. 10.069 0.29224 F093001000080 2.39 125. 10.093 0.27375 F093001000081 2.39 125. 10.103 0.31695 F093001000082 2.39 125. 10.121 0.30669 F093001000083 2.39 125. 10.125 0.24705 F093001000084 2.39 125. 10.145 0.30671 F093001000085 2.39 125. 10.153 0.26559 F093001000086 2.39 125. 10.165 0.32112 F093001000087 2.39 125. 10.178 0.27383 F093001000088 2.39 125. 10.182 0.41163 F093001000089 2.39 125. 10.198 0.50213 F093001000090 2.39 125. 10.209 0.75921 F093001000091 2.39 125. 10.223 0.90524 F093001000092 2.39 125. 10.233 0.88057 F093001000093 2.39 125. 10.24 0.74485 F093001000094 2.39 125. 10.246 0.59678 F093001000095 2.39 125. 10.26 0.5351 F093001000096 2.39 125. 10.266 0.45901 F093001000097 2.39 125. 10.272 0.41788 F093001000098 2.39 125. 10.284 0.38499 F093001000099 2.39 125. 10.298 0.35827 F093001000100 2.39 125. 10.308 0.34183 F093001000101 2.39 125. 10.323 0.31305 F093001000102 2.39 125. 10.339 0.31718 F093001000103 2.39 125. 10.343 0.27399 F093001000104 2.39 125. 10.355 0.27401 F093001000105 2.39 125. 10.371 0.27813 F093001000106 2.39 125. 10.385 0.29049 F093001000107 2.39 125. 10.393 0.25965 F093001000108 2.39 125. 10.407 0.26583 F093001000109 2.39 125. 10.415 0.23705 F093001000110 2.39 125. 10.425 0.27819 F093001000111 ENDDATA 85 0 F093001000112 ENDSUBENT 111 0 F093001099999 SUBENT F0930011 20080528 F032F093001100001 BIB 6 17 F093001100002 REACTION (50-SN-122(P,INL)50-SN-122,PAR,DA) F093001100003 MONITOR The absolute cross sections were obtained by F093001100004 determining the target thickness from 4 MeV cross F093001100005 section data at forward angles where Rutherford F093001100006 scattering predominates. F093001100007 DETECTOR (SILI) 2 mm Si(Li) detectors. F093001100008 (SIBAR) 2 mm surface-barrier detectors. Each detector F093001100009 was mounted with a collimator and anti-scattering F093001100010 baffle on a plate which could be rotated. The angular F093001100011 acceptance was +-1.1 degr. F093001100012 SAMPLE Targets with approximately 300 mu-g/cm2 of tin on 10 F093001100013 mu-g/cm2 of carbon backing were used. F093001100014 ERR-ANALYS The uncertainty in the absolute cross section was F093001100015 estimated to be 5% F093001100016 (EN-ERR-DIG) Energy digitizing error F093001100017 (DATA-ERR) Error from the graphic bars F093001100018 STATUS (CURVE)Fig.5 F093001100019 ENDBIB 17 0 F093001100020 COMMON 2 3 F093001100021 EN-ERR-DIG ERR-DIG F093001100022 MEV MB/SR F093001100023 0.0003 0.0009 F093001100024 ENDCOMMON 3 0 F093001100025 DATA 5 68 F093001100026 E-LVL ANG EN DATA DATA-ERR F093001100027 MEV ADEG MEV MB/SR MB/SR F093001100028 1.14 140. 10.102 0.14801 F093001100029 1.14 140. 10.123 0.1683 F093001100030 1.14 140. 10.135 9.9392E-02 F093001100031 1.14 140. 10.155 0.12779 F093001100032 1.14 140. 10.184 0.12984 F093001100033 1.14 140. 10.202 0.13188 F093001100034 1.14 140. 10.222 0.17243 F093001100035 1.14 140. 10.242 0.14002 F093001100036 1.14 140. 10.263 9.3413E-02 F093001100037 1.14 140. 10.283 0.11167 F093001100038 1.14 140. 10.303 0.12385 F093001100039 1.14 140. 10.318 0.13805 F093001100040 1.14 140. 10.334 0.20496 F093001100041 1.14 140. 10.358 0.132 F093001100042 1.14 140. 10.381 0.17053 F093001100043 1.14 140. 10.401 0.17258 F093001100044 1.14 140. 10.419 0.14827 F093001100045 1.14 140. 10.43 0.23341 F093001100046 1.14 140. 10.46 0.33073 F093001100047 1.14 140. 10.481 0.47061 F093001100048 1.14 140. 10.501 0.58617 F093001100049 1.14 140. 10.519 0.56997 F093001100050 1.14 140. 10.533 0.28417 F093001100051 1.14 140. 10.554 0.3004 F093001100052 1.14 140. 10.578 0.27812 F093001100053 1.14 140. 10.6 0.17882 F093001100054 1.14 140. 10.619 0.23762 F093001100055 1.14 140. 10.639 0.23966 F093001100056 1.14 140. 10.662 0.2417 F093001100057 1.14 140. 10.68 0.18902 F093001100058 1.14 140. 10.702 0.18903 F093001100059 1.14 140. 10.723 0.22148 F093001100060 1.14 140. 10.741 0.23569 F093001100061 1.14 140. 10.755 0.1607 F093001100062 1.14 140. 10.78 0.22761 F093001100063 2.54 120. 10.104 7.4315E-02 F093001100064 2.54 120. 10.126 5.1671E-02 F093001100065 2.54 120. 10.152 5.5837E-02 F093001100066 2.54 120. 10.166 4.3489E-02 F093001100067 2.54 120. 10.184 5.1765E-02 F093001100068 2.54 120. 10.204 3.7365E-02 F093001100069 2.54 120. 10.222 4.9766E-02 F093001100070 2.54 120. 10.245 0.10135 F093001100071 2.54 120. 10.265 9.1075E-02 F093001100072 2.54 120. 10.283 0.12409 F093001100073 2.54 120. 10.305 0.1097 3.5051E-02 F093001100074 2.54 120. 10.323 0.1056 F093001100075 2.54 120. 10.367 0.10361 F093001100076 2.54 120. 10.387 0.11395 F093001100077 2.54 120. 10.409 0.1511 F093001100078 2.54 120. 10.429 0.1965 F093001100079 2.54 120. 10.448 0.39241 F093001100080 2.54 120. 10.464 0.49552 F093001100081 2.54 120. 10.488 0.50381 F093001100082 2.54 120. 10.504 0.41105 F093001100083 2.54 120. 10.526 0.3348 F093001100084 2.54 120. 10.546 0.30391 F093001100085 2.54 120. 10.564 0.11425 F093001100086 2.54 120. 10.586 0.11841 F093001100087 2.54 120. 10.604 0.10813 F093001100088 2.54 120. 10.624 0.12465 F093001100089 2.54 120. 10.644 5.8707E-02 F093001100090 2.54 120. 10.664 7.3173E-02 F093001100091 2.54 120. 10.684 0.1165 F093001100092 2.54 120. 10.7 7.9417E-02 F093001100093 2.54 120. 10.72 0.10007 F093001100094 2.54 120. 10.742 5.2682E-02 F093001100095 2.54 120. 10.764 7.5398E-02 F093001100096 ENDDATA 70 0 F093001100097 ENDSUBENT 96 0 F093001199999 SUBENT F0930012 20080528 F032F093001200001 BIB 6 16 F093001200002 REACTION (50-SN-124(P,INL)50-SN-124,PAR,DA) F093001200003 MONITOR The absolute cross sections were obtained by F093001200004 determining the target thickness from 4 MeV cross F093001200005 section data at forward angles where Rutherford F093001200006 scattering predominates. F093001200007 DETECTOR (SILI) 2 mm Si(Li) detectors. F093001200008 (SIBAR) 2 mm surface-barrier detectors. Each detector F093001200009 was mounted with a collimator and anti-scattering F093001200010 baffle on a plate which could be rotated. The angular F093001200011 acceptance was +-1.1 degr. F093001200012 SAMPLE Targets with approximately 300 mu-g/cm2 of tin on 10 F093001200013 mu-g/cm2 of carbon backing were used. F093001200014 ERR-ANALYS The uncertainty in the absolute cross section was F093001200015 estimated to be 5% F093001200016 (EN-ERR-DIG) Energy digitizing error F093001200017 STATUS (CURVE)Fig.5 F093001200018 ENDBIB 16 0 F093001200019 COMMON 2 3 F093001200020 EN-ERR-DIG ERR-DIG F093001200021 MEV MB/SR F093001200022 0.0007 0.0001 F093001200023 ENDCOMMON 3 0 F093001200024 DATA 4 45 F093001200025 E-LVL ANG EN DATA F093001200026 MEV ADEG MEV MB/SR F093001200027 1.13 130. 10.296 0.2343 F093001200028 1.13 130. 10.352 0.17946 F093001200029 1.13 130. 10.399 0.21802 F093001200030 1.13 130. 10.451 0.26673 F093001200031 1.13 130. 10.5 0.26874 F093001200032 1.13 130. 10.516 0.29919 F093001200033 1.13 130. 10.54 0.29715 F093001200034 1.13 130. 10.561 0.31948 F093001200035 1.13 130. 10.575 0.38648 F093001200036 1.13 130. 10.599 0.50018 F093001200037 1.13 130. 10.619 0.70321 F093001200038 1.13 130. 10.643 0.85143 F093001200039 1.13 130. 10.665 0.89 F093001200040 1.13 130. 10.68 0.63213 F093001200041 1.13 130. 10.702 0.46968 F093001200042 1.13 130. 10.724 0.39658 F093001200043 1.13 130. 10.742 0.33769 F093001200044 1.13 130. 10.761 0.31738 F093001200045 1.13 130. 10.781 0.30722 F093001200046 1.13 130. 10.803 0.31736 F093001200047 1.13 130. 10.821 0.32751 F093001200048 1.13 130. 10.853 0.31532 F093001200049 1.13 130. 10.902 0.30718 F093001200050 2.59 130. 10.353 0.11338 F093001200051 2.59 130. 10.405 0.14223 F093001200052 2.59 130. 10.455 0.13191 F093001200053 2.59 130. 10.501 7.8292E-02 F093001200054 2.59 130. 10.521 0.11952 F093001200055 2.59 130. 10.539 0.12983 F093001200056 2.59 130. 10.563 0.15457 F093001200057 2.59 130. 10.583 0.20198 F093001200058 2.59 130. 10.606 0.20198 F093001200059 2.59 130. 10.624 0.26796 F093001200060 2.59 130. 10.644 0.30094 F093001200061 2.59 130. 10.664 0.27413 F093001200062 2.59 130. 10.684 0.22052 F093001200063 2.59 130. 10.706 0.21227 F093001200064 2.59 130. 10.724 0.23907 F093001200065 2.59 130. 10.748 0.21844 F093001200066 2.59 130. 10.768 0.20194 F093001200067 2.59 130. 10.79 0.17307 F093001200068 2.59 130. 10.808 0.15657 F093001200069 2.59 130. 10.828 0.16069 F093001200070 2.59 130. 10.854 0.16893 F093001200071 2.59 130. 10.908 0.16892 F093001200072 ENDDATA 47 0 F093001200073 ENDSUBENT 72 0 F093001299999 ENDENTRY 12 0 F093099999999