ENTRY C1850 20180315 C174C185000000001 SUBENT C1850001 20180315 C174C185000100001 BIB 6 8 C185000100002 TITLE A search for an excited state of B9 near 1.7 MeV C185000100003 AUTHOR (R.W.Bauer,J.D.Anderson,C.Wong) C185000100004 REFERENCE (J,NP,56,117,1964) C185000100005 #doi:10.1016/0029-5582(64)90458-4 C185000100006 INSTITUTE (1USALRL) C185000100007 FACILITY (CYCLO,1USALRL) Livermore 230 cm variable energy C185000100008 cyclotron. C185000100009 HISTORY (20180315C) BP C185000100010 ENDBIB 8 0 C185000100011 NOCOMMON 0 0 C185000100012 ENDSUBENT 11 0 C185000199999 SUBENT C1850002 20180315 C174C185000200001 BIB 5 18 C185000200002 REACTION (6-C-12(P,X)2-HE-4,,DA/DE) C185000200003 SAMPLE A thin self-supported polystyrene (CH) target located C185000200004 at the center of a 1 m diam. scattering chamber. C185000200005 Targets of thicknesses ranging from 50 to C185000200006 150 microg/cm2 were used. C185000200007 DETECTOR (SIBAR) The alpha spectra were measured using a thin C185000200008 Ortec Surface Barrier detector (50 microm thickness, C185000200009 totally depleted at a reverse bias of about 100 V). C185000200010 ERR-ANALYS (DATA-ERR) The absolute differential cross sections C185000200011 for the ground state group are accurate to within C185000200012 about 25%. The large uncertainty is due to the fact C185000200013 that the usual precautions with regard to charge C185000200014 collection have not been carefully observed since the C185000200015 main emphasis in this experiment was on energy C185000200016 spectra. In those cases where the continuous spectra C185000200017 are well described by the four-body shape, the C185000200018 breakup cross section is accurate to within 25 %. C185000200019 STATUS (CURVE) Fig. 1, page 121. C185000200020 ENDBIB 18 0 C185000200021 COMMON 2 3 C185000200022 EN ANG C185000200023 MEV ADEG C185000200024 12.7 45.0 C185000200025 ENDCOMMON 3 0 C185000200026 DATA 3 39 C185000200027 E-CM DATA-CM DATA-ERR C185000200028 MEV MB/SR/MEV MB/SR/MEV C185000200029 1.234 5.984E+00 2.496E-01 C185000200030 1.310 6.070E+00 3.352E-01 C185000200031 1.416 5.735E+00 3.931E-01 C185000200032 1.447 5.342E+00 C185000200033 1.477 4.975E+00 C185000200034 1.568 4.975E+00 C185000200035 1.644 5.047E+00 3.459E-01 C185000200036 1.705 4.768E+00 1.989E-01 C185000200037 1.750 4.701E+00 C185000200038 1.826 4.634E+00 1.933E-01 C185000200039 1.857 4.317E+00 C185000200040 1.902 4.317E+00 2.384E-01 C185000200041 1.948 4.137E+00 2.284E-01 C185000200042 2.008 3.692E+00 2.039E-01 C185000200043 2.039 3.343E+00 2.291E-01 C185000200044 2.115 2.860E+00 1.960E-01 C185000200045 2.145 2.446E+00 C185000200046 2.191 2.122E+00 1.455E-01 C185000200047 2.221 1.977E+00 C185000200048 2.251 1.841E+00 C185000200049 2.297 1.644E+00 C185000200050 2.327 1.426E+00 5.947E-02 C185000200051 2.358 1.273E+00 C185000200052 2.418 1.237E+00 8.480E-02 C185000200053 2.464 1.220E+00 8.360E-02 C185000200054 2.525 7.212E-01 3.983E-02 C185000200055 2.631 5.507E-01 3.041E-02 C185000200056 2.737 5.828E-01 C185000200057 2.752 9.052E-01 4.999E-02 C185000200058 2.783 2.005E+00 C185000200059 2.783 3.745E+00 C185000200060 2.798 1.027E+01 C185000200061 2.843 1.443E+01 C185000200062 2.919 1.252E+01 C185000200063 2.965 6.610E+00 C185000200064 3.026 2.626E+00 C185000200065 3.056 6.257E-01 C185000200066 3.086 4.204E-01 C185000200067 3.147 1.060E-01 C185000200068 ENDDATA 41 0 C185000200069 ENDSUBENT 68 0 C185000299999 SUBENT C1850003 20180315 C174C185000300001 BIB 5 18 C185000300002 REACTION (6-C-12(P,X)2-HE-4,,DA/DE) C185000300003 SAMPLE A thin self-supported polystyrene (CH) target located C185000300004 at the center of a 1 m diam. scattering chamber. C185000300005 Targets of thicknesses ranging from 50 to C185000300006 150 microg/cm2 were used. C185000300007 DETECTOR (SIBAR) The alpha spectra were measured using a thin C185000300008 Ortec Surface Barrier detector (50 microm thickness, C185000300009 totally depleted at a reverse bias of about 100 V). C185000300010 ERR-ANALYS (DATA-ERR) The absolute differential cross sections C185000300011 for the ground state group are accurate to within C185000300012 about 25%. The large uncertainty is due to the fact C185000300013 that the usual precautions with regard to charge C185000300014 collection have not been carefully observed since the C185000300015 main emphasis in this experiment was on energy C185000300016 spectra. In those cases where the continuous spectra C185000300017 are well described by the four-body shape, the C185000300018 breakup cross section is accurate to within 25 %. C185000300019 STATUS (CURVE) Fig. 1, page 121. C185000300020 ENDBIB 18 0 C185000300021 COMMON 2 3 C185000300022 EN ANG C185000300023 MEV ADEG C185000300024 14.3 86.0 C185000300025 ENDCOMMON 3 0 C185000300026 DATA 3 35 C185000300027 E-CM DATA-CM DATA-ERR C185000300028 MEV MB/SR/MEV MB/SR/MEV C185000300029 2.115 6.274E+00 C185000300030 2.160 6.013E+00 C185000300031 2.236 5.005E+00 C185000300032 2.282 3.992E+00 C185000300033 2.327 3.010E+00 C185000300034 2.403 2.367E+00 C185000300035 2.449 2.085E+00 C185000300036 2.525 1.862E+00 1.023E-01 C185000300037 2.585 1.785E+00 9.804E-02 C185000300038 2.646 1.572E+00 8.633E-02 C185000300039 2.707 1.572E+00 1.072E-01 C185000300040 2.752 1.404E+00 9.571E-02 C185000300041 2.813 1.271E+00 5.276E-02 C185000300042 2.904 1.136E+00 C185000300043 2.965 9.860E-01 5.417E-02 C185000300044 3.041 1.043E+00 5.732E-02 C185000300045 3.102 7.977E-01 C185000300046 3.177 6.829E-01 2.834E-02 C185000300047 3.238 7.125E-01 4.859E-02 C185000300048 3.284 6.099E-01 4.957E-02 C185000300049 3.329 6.186E-01 4.218E-02 C185000300050 3.345 4.598E-01 3.737E-02 C185000300051 3.420 4.664E-01 3.790E-02 C185000300052 3.466 4.470E-01 2.456E-02 C185000300053 3.542 4.534E-01 2.491E-02 C185000300054 3.603 4.407E-01 2.421E-02 C185000300055 3.633 5.604E-01 C185000300056 3.739 2.334E+00 C185000300057 3.770 4.470E+00 C185000300058 3.815 6.829E+00 C185000300059 3.876 7.865E+00 C185000300060 3.967 4.598E+00 C185000300061 4.013 2.026E+00 C185000300062 4.073 5.076E-01 C185000300063 4.134 7.755E-02 C185000300064 ENDDATA 37 0 C185000300065 ENDSUBENT 64 0 C185000399999 SUBENT C1850004 20180315 C174C185000400001 BIB 5 18 C185000400002 REACTION (6-C-12(P,X)2-HE-4,,DA/DE) C185000400003 SAMPLE A thin self-supported polystyrene (CH) target located C185000400004 at the center of a 1 m diam. scattering chamber. C185000400005 Targets of thicknesses ranging from 50 to C185000400006 150 microg/cm2 were used. C185000400007 DETECTOR (SIBAR) The alpha spectra were measured using a thin C185000400008 Ortec Surface Barrier detector (50 microm thickness, C185000400009 totally depleted at a reverse bias of about 100 V). C185000400010 ERR-ANALYS (DATA-ERR) The absolute differential cross sections C185000400011 for the ground state group are accurate to within C185000400012 about 25%. The large uncertainty is due to the fact C185000400013 that the usual precautions with regard to charge C185000400014 collection have not been carefully observed since the C185000400015 main emphasis in this experiment was on energy C185000400016 spectra. In those cases where the continuous spectra C185000400017 are well described by the four-body shape, the C185000400018 breakup cross section is accurate to within 25 %. C185000400019 STATUS (CURVE) Fig. 1, page 121. C185000400020 ENDBIB 18 0 C185000400021 COMMON 2 3 C185000400022 EN ANG C185000400023 MEV ADEG C185000400024 16.0 90.0 C185000400025 ENDCOMMON 3 0 C185000400026 DATA 3 64 C185000400027 E-CM DATA-CM DATA-ERR C185000400028 MEV MB/SR/MEV MB/SR/MEV C185000400029 2.175 9.047E+00 5.030E-01 C185000400030 2.206 8.303E+00 C185000400031 2.251 8.069E+00 3.389E-01 C185000400032 2.297 7.197E+00 3.023E-01 C185000400033 2.342 7.621E+00 4.237E-01 C185000400034 2.403 7.301E+00 3.066E-01 C185000400035 2.433 6.700E+00 1.889E-01 C185000400036 2.494 6.328E+00 3.518E-01 C185000400037 2.525 5.725E+00 1.614E-01 C185000400038 2.540 5.330E+00 2.963E-01 C185000400039 2.570 4.620E+00 3.188E-01 C185000400040 2.631 4.554E+00 2.532E-01 C185000400041 2.676 4.363E+00 2.426E-01 C185000400042 2.722 4.240E+00 2.926E-01 C185000400043 2.798 4.240E+00 2.357E-01 C185000400044 2.874 4.120E+00 2.291E-01 C185000400045 2.919 4.120E+00 2.291E-01 C185000400046 2.950 3.728E+00 2.073E-01 C185000400047 3.026 3.836E+00 2.133E-01 C185000400048 3.071 3.622E+00 2.500E-01 C185000400049 3.162 3.781E+00 2.610E-01 C185000400050 3.193 4.962E+00 C185000400051 3.223 7.301E+00 C185000400052 3.269 1.059E+01 C185000400053 3.329 1.137E+01 C185000400054 3.375 1.044E+01 C185000400055 3.420 6.895E+00 C185000400056 3.496 3.781E+00 C185000400057 3.527 2.498E+00 C185000400058 3.618 1.850E+00 C185000400059 3.663 1.370E+00 5.753E-02 C185000400060 3.724 1.430E+00 C185000400061 3.754 1.275E+00 7.090E-02 C185000400062 3.800 1.121E+00 3.162E-02 C185000400063 3.846 1.257E+00 8.676E-02 C185000400064 3.921 1.074E+00 5.972E-02 C185000400065 3.937 1.187E+00 6.601E-02 C185000400066 3.997 9.178E-01 6.334E-02 C185000400067 4.043 9.444E-01 3.966E-02 C185000400068 4.058 1.074E+00 5.972E-02 C185000400069 4.119 9.718E-01 2.740E-02 C185000400070 4.180 8.303E-01 6.828E-02 C185000400071 4.225 9.047E-01 5.030E-02 C185000400072 4.256 7.621E-01 4.237E-02 C185000400073 4.316 7.955E-01 6.541E-02 C185000400074 4.347 6.895E-01 C185000400075 4.423 6.328E-01 1.784E-02 C185000400076 4.423 6.994E-01 3.889E-02 C185000400077 4.468 6.062E-01 C185000400078 4.514 5.976E-01 4.914E-02 C185000400079 4.574 5.807E-01 4.008E-02 C185000400080 4.635 5.725E-01 3.183E-02 C185000400081 4.681 4.822E-01 3.328E-02 C185000400082 4.757 5.563E-01 C185000400083 4.757 4.822E-01 3.328E-02 C185000400084 4.817 9.718E-01 C185000400085 4.863 2.721E+00 C185000400086 4.893 7.301E+00 C185000400087 4.939 9.718E+00 C185000400088 4.969 1.029E+01 C185000400089 5.000 1.059E+01 C185000400090 5.045 6.895E+00 C185000400091 5.091 2.761E+00 C185000400092 5.136 5.254E-01 C185000400093 ENDDATA 66 0 C185000400094 ENDSUBENT 93 0 C185000499999 SUBENT C1850005 20180315 C174C185000500001 BIB 5 18 C185000500002 REACTION (6-C-12(P,X)2-HE-4,,DA/DE) C185000500003 SAMPLE A thin self-supported polystyrene (CH) target located C185000500004 at the center of a 1 m diam. scattering chamber. C185000500005 Targets of thicknesses ranging from 50 to C185000500006 150 microg/cm2 were used. C185000500007 DETECTOR (SIBAR) The alpha spectra were measured using a thin C185000500008 Ortec Surface Barrier detector (50 microm thickness, C185000500009 totally depleted at a reverse bias of about 100 V). C185000500010 ERR-ANALYS (DATA-ERR) The absolute differential cross sections C185000500011 for the ground state group are accurate to within C185000500012 about 25%. The large uncertainty is due to the fact C185000500013 that the usual precautions with regard to charge C185000500014 collection have not been carefully observed since the C185000500015 main emphasis in this experiment was on energy C185000500016 spectra. In those cases where the continuous spectra C185000500017 are well described by the four-body shape, the C185000500018 breakup cross section is accurate to within 25 %. C185000500019 STATUS (CURVE) Fig. 1, page 121. C185000500020 ENDBIB 18 0 C185000500021 COMMON 2 3 C185000500022 EN ANG C185000500023 MEV ADEG C185000500024 18.3 90.0 C185000500025 ENDCOMMON 3 0 C185000500026 DATA 3 57 C185000500027 E-CM DATA-CM DATA-ERR C185000500028 MEV MB/SR/MEV MB/SR/MEV C185000500029 3.679 5.148E+00 C185000500030 3.694 5.371E+00 4.751E-01 C185000500031 3.770 5.296E+00 3.611E-01 C185000500032 3.876 4.598E+00 3.136E-01 C185000500033 3.937 4.407E+00 3.006E-01 C185000500034 3.982 3.827E+00 1.588E-01 C185000500035 4.028 3.881E+00 2.132E-01 C185000500036 4.089 3.827E+00 3.110E-01 C185000500037 4.134 3.720E+00 2.044E-01 C185000500038 4.210 3.773E+00 2.573E-01 C185000500039 4.256 3.566E+00 C185000500040 4.301 3.566E+00 2.432E-01 C185000500041 4.347 3.096E+00 1.701E-01 C185000500042 4.377 3.276E+00 1.800E-01 C185000500043 4.453 3.096E+00 2.111E-01 C185000500044 4.529 3.466E+00 1.904E-01 C185000500045 4.650 3.185E+00 2.172E-01 C185000500046 4.726 4.470E+00 C185000500047 4.772 5.683E+00 C185000500048 4.832 6.546E+00 C185000500049 4.863 7.125E+00 C185000500050 4.908 6.926E+00 C185000500051 4.924 6.274E+00 C185000500052 4.984 4.797E+00 C185000500053 5.030 3.773E+00 C185000500054 5.091 2.175E+00 C185000500055 5.121 1.345E+00 C185000500056 5.151 1.058E+00 C185000500057 5.197 6.639E-01 5.395E-02 C185000500058 5.258 6.274E-01 3.447E-02 C185000500059 5.288 5.846E-01 8.200E-03 C185000500060 5.334 7.025E-01 4.790E-02 C185000500061 5.379 5.296E-01 C185000500062 5.425 4.935E-01 3.365E-02 C185000500063 5.501 5.148E-01 C185000500064 5.516 4.470E-01 2.456E-02 C185000500065 5.561 4.730E-01 3.844E-02 C185000500066 5.607 4.165E-01 2.840E-02 C185000500067 5.713 4.470E-01 2.456E-02 C185000500068 5.744 3.185E-01 2.172E-02 C185000500069 5.850 2.144E-01 1.462E-02 C185000500070 5.865 3.185E-01 2.172E-02 C185000500071 5.971 2.470E-01 1.684E-02 C185000500072 6.062 1.942E-01 1.325E-02 C185000500073 6.108 3.370E-01 2.298E-02 C185000500074 6.199 3.010E-01 C185000500075 6.245 6.829E-01 C185000500076 6.305 1.862E+00 C185000500077 6.351 3.140E+00 C185000500078 6.381 4.663E+00 C185000500079 6.396 5.604E+00 C185000500080 6.472 6.639E+00 C185000500081 6.609 6.099E+00 C185000500082 6.655 3.881E+00 C185000500083 6.700 1.345E+00 C185000500084 6.700 4.165E-01 C185000500085 6.791 5.764E-02 C185000500086 ENDDATA 59 0 C185000500087 ENDSUBENT 86 0 C185000599999 SUBENT C1850006 20180315 C174C185000600001 BIB 4 9 C185000600002 REACTION (6-C-12(P,X)2-HE-4,,DA/DE) C185000600003 SAMPLE A thin self-supported polystyrene (CH) target located C185000600004 at the center of a 1 m diam. scattering chamber. C185000600005 Targets of thicknesses ranging from 50 to C185000600006 150 microg/cm2 were used. C185000600007 DETECTOR (SIBAR) The alpha spectra were measured using a thin C185000600008 Ortec Surface Barrier detector (50 microm thickness, C185000600009 totally depleted at a reverse bias of about 100 V). C185000600010 STATUS (CURVE) Fig. 2, page 122. C185000600011 ENDBIB 9 0 C185000600012 COMMON 2 3 C185000600013 EN ANG C185000600014 MEV ADEG C185000600015 14.3 41.0 C185000600016 ENDCOMMON 3 0 C185000600017 DATA 2 87 C185000600018 E-CM DATA-CM C185000600019 MEV MB/SR/MEV C185000600020 1.431 4.587E+00 C185000600021 1.475 5.038E+00 C185000600022 1.487 4.430E+00 C185000600023 1.537 4.329E+00 C185000600024 1.581 4.279E+00 C185000600025 1.612 4.645E+00 C185000600026 1.655 4.592E+00 C185000600027 1.674 4.812E+00 C185000600028 1.686 4.647E+00 C185000600029 1.730 4.870E+00 C185000600030 1.730 4.332E+00 C185000600031 1.780 4.929E+00 C185000600032 1.805 4.704E+00 C185000600033 1.836 4.760E+00 C185000600034 1.873 4.651E+00 C185000600035 1.873 4.285E+00 C185000600036 1.898 4.651E+00 C185000600037 1.911 4.762E+00 C185000600038 1.954 4.492E+00 C185000600039 1.985 4.440E+00 C185000600040 2.023 4.288E+00 C185000600041 2.035 4.654E+00 C185000600042 2.041 4.189E+00 C185000600043 2.079 3.998E+00 C185000600044 2.110 4.656E+00 C185000600045 2.147 4.767E+00 C185000600046 2.160 4.995E+00 C185000600047 2.172 5.682E+00 C185000600048 2.172 5.359E+00 C185000600049 2.190 6.096E+00 C185000600050 2.209 6.539E+00 C185000600051 2.240 6.934E+00 C185000600052 2.278 6.542E+00 C185000600053 2.290 6.170E+00 C185000600054 2.296 5.888E+00 C185000600055 2.309 5.619E+00 C185000600056 2.321 5.239E+00 C185000600057 2.334 4.941E+00 C185000600058 2.346 4.500E+00 C185000600059 2.353 3.957E+00 C185000600060 2.372 3.646E+00 C185000600061 2.384 3.480E+00 C185000600062 2.384 3.282E+00 C185000600063 2.397 3.096E+00 C185000600064 2.409 2.819E+00 C185000600065 2.435 2.366E+00 C185000600066 2.472 2.232E+00 C185000600067 2.522 1.963E+00 C185000600068 2.547 1.726E+00 C185000600069 2.597 1.767E+00 C185000600070 2.628 1.609E+00 C185000600071 2.684 1.610E+00 C185000600072 2.715 1.501E+00 C185000600073 2.765 1.450E+00 C185000600074 2.796 1.688E+00 C185000600075 2.840 1.433E+00 C185000600076 2.884 1.275E+00 C185000600077 2.927 1.417E+00 C185000600078 2.971 1.451E+00 C185000600079 3.002 1.122E+00 C185000600080 3.039 1.176E+00 C185000600081 3.096 1.084E+00 C185000600082 3.133 1.084E+00 C185000600083 3.177 8.579E-01 C185000600084 3.214 9.204E-01 C185000600085 3.264 6.952E-01 C185000600086 3.289 6.872E-01 C185000600087 3.345 6.955E-01 C185000600088 3.383 6.335E-01 C185000600089 3.433 6.118E-01 C185000600090 3.477 4.675E-01 C185000600091 3.514 4.515E-01 C185000600092 3.539 3.745E-01 C185000600093 3.639 3.617E-01 C185000600094 3.689 3.576E-01 C185000600095 3.701 3.704E-01 C185000600096 3.726 4.020E-01 C185000600097 3.762 8.909E-01 C185000600098 3.798 3.008E+00 C185000600099 3.847 6.363E+00 C185000600100 3.896 8.627E+00 C185000600101 3.946 7.766E+00 C185000600102 3.978 5.157E+00 C185000600103 4.028 2.711E+00 C185000600104 4.055 9.683E-01 C185000600105 4.094 2.351E-01 C185000600106 4.158 8.110E-02 C185000600107 ENDDATA 89 0 C185000600108 ENDSUBENT 107 0 C185000699999 SUBENT C1850007 20180315 C174C185000700001 BIB 5 18 C185000700002 REACTION (6-C-12(P,X)2-HE-4,,DA/DE) C185000700003 SAMPLE A thin self-supported polystyrene (CH) target located C185000700004 at the center of a 1 m diam. scattering chamber. C185000700005 Targets of thicknesses ranging from 50 to C185000700006 150 microg/cm2 were used. C185000700007 DETECTOR (SIBAR) The alpha spectra were measured using a thin C185000700008 Ortec Surface Barrier detector (50 microm thickness, C185000700009 totally depleted at a reverse bias of about 100 V). C185000700010 ERR-ANALYS (DATA-ERR) The absolute differential cross sections C185000700011 for the ground state group are accurate to within C185000700012 about 25%. The large uncertainty is due to the fact C185000700013 that the usual precautions with regard to charge C185000700014 collection have not been carefully observed since the C185000700015 main emphasis in this experiment was on energy C185000700016 spectra. In those cases where the continuous spectra C185000700017 are well described by the four-body shape, the C185000700018 breakup cross section is accurate to within 25 %. C185000700019 STATUS (CURVE) Fig. 3, page 123. C185000700020 ENDBIB 18 0 C185000700021 COMMON 2 3 C185000700022 EN ANG C185000700023 MEV ADEG C185000700024 16.0 22.0 C185000700025 ENDCOMMON 3 0 C185000700026 DATA 3 84 C185000700027 E-CM DATA-CM DATA-ERR C185000700028 MEV MB/SR/MEV MB/SR/MEV C185000700029 2.093 9.981E+00 7.492E-01 C185000700030 2.115 9.363E+00 5.791E-01 C185000700031 2.153 9.633E+00 4.014E-01 C185000700032 2.183 8.722E+00 4.812E-01 C185000700033 2.235 8.359E+00 4.049E-01 C185000700034 2.280 8.183E+00 4.514E-01 C185000700035 2.288 9.166E+00 4.440E-01 C185000700036 2.355 8.910E+00 3.713E-01 C185000700037 2.385 8.538E+00 4.711E-01 C185000700038 2.438 7.462E+00 5.110E-01 C185000700039 2.490 7.568E+00 5.183E-01 C185000700040 2.543 7.409E+00 4.582E-01 C185000700041 2.580 6.804E+00 5.108E-01 C185000700042 2.655 6.614E+00 4.529E-01 C185000700043 2.685 5.989E+00 3.704E-01 C185000700044 2.745 6.031E+00 4.130E-01 C185000700045 2.775 5.234E+00 2.887E-01 C185000700046 2.820 5.946E+00 4.072E-01 C185000700047 2.858 6.031E+00 3.730E-01 C185000700048 2.880 5.271E+00 3.260E-01 C185000700049 2.918 5.346E+00 3.661E-01 C185000700050 2.963 4.980E+00 3.080E-01 C185000700051 3.008 5.087E+00 2.807E-01 C185000700052 3.068 4.773E+00 2.952E-01 C185000700053 3.113 4.807E+00 3.292E-01 C185000700054 3.165 4.807E+00 2.973E-01 C185000700055 3.218 4.739E+00 2.931E-01 C185000700056 3.248 5.051E+00 C185000700057 3.293 5.234E+00 C185000700058 3.293 5.500E+00 C185000700059 3.345 5.780E+00 C185000700060 3.368 6.338E+00 C185000700061 3.375 6.661E+00 C185000700062 3.390 7.202E+00 C185000700063 3.405 7.622E+00 C185000700064 3.450 7.151E+00 C185000700065 3.465 6.521E+00 C185000700066 3.503 5.821E+00 C185000700067 3.510 5.016E+00 C185000700068 3.518 5.308E+00 2.572E-01 C185000700069 3.548 4.672E+00 C185000700070 3.563 4.291E+00 2.654E-01 C185000700071 3.578 3.568E+00 2.678E-01 C185000700072 3.593 2.172E+00 1.198E-01 C185000700073 3.600 3.074E+00 C185000700074 3.660 2.298E+00 1.268E-01 C185000700075 3.735 1.939E+00 9.391E-02 C185000700076 3.765 2.009E+00 1.108E-01 C185000700077 3.825 1.980E+00 1.225E-01 C185000700078 3.893 1.743E+00 9.616E-02 C185000700079 3.900 1.429E+00 7.884E-02 C185000700080 3.953 1.635E+00 1.011E-01 C185000700081 4.013 1.601E+00 9.900E-02 C185000700082 4.073 1.491E+00 8.226E-02 C185000700083 4.125 1.341E+00 7.396E-02 C185000700084 4.178 1.360E+00 8.410E-02 C185000700085 4.230 1.084E+00 7.420E-02 C185000700086 4.283 1.017E+00 6.962E-02 C185000700087 4.313 1.053E+00 8.595E-02 C185000700088 4.373 1.009E+00 7.577E-02 C185000700089 4.410 9.952E-01 9.408E-02 C185000700090 4.440 8.884E-01 5.495E-02 C185000700091 4.478 7.600E-01 4.701E-02 C185000700092 4.508 6.410E-01 3.537E-02 C185000700093 4.523 8.217E-01 5.627E-02 C185000700094 4.568 7.232E-01 4.473E-02 C185000700095 4.620 6.785E-01 4.646E-02 C185000700096 4.635 6.057E-01 4.148E-02 C185000700097 4.673 5.109E-01 2.818E-02 C185000700098 4.733 4.692E-01 3.829E-02 C185000700099 4.733 5.763E-01 5.449E-02 C185000700100 4.808 4.593E-01 4.046E-02 C185000700101 4.830 6.143E-01 C185000700102 4.883 9.811E-01 C185000700103 4.913 2.081E+00 C185000700104 4.965 5.123E+00 C185000700105 4.973 8.784E+00 C185000700106 5.040 1.235E+01 C185000700107 5.123 9.101E+00 C185000700108 5.168 5.618E+00 C185000700109 5.198 2.485E+00 C185000700110 5.228 1.214E+00 C185000700111 5.280 3.508E-01 C185000700112 5.317 1.254E-01 C185000700113 ENDDATA 86 0 C185000700114 ENDSUBENT 113 0 C185000799999 SUBENT C1850008 20180315 C174C185000800001 BIB 5 18 C185000800002 REACTION (6-C-12(P,X)2-HE-4,,DA/DE) C185000800003 SAMPLE A thin self-supported polystyrene (CH) target located C185000800004 at the center of a 1 m diam. scattering chamber. C185000800005 Targets of thicknesses ranging from 50 to C185000800006 150 microg/cm2 were used. C185000800007 DETECTOR (SIBAR) The alpha spectra were measured using a thin C185000800008 Ortec Surface Barrier detector (50 microm thickness, C185000800009 totally depleted at a reverse bias of about 100 V). C185000800010 ERR-ANALYS (DATA-ERR) The absolute differential cross sections C185000800011 for the ground state group are accurate to within C185000800012 about 25%. The large uncertainty is due to the fact C185000800013 that the usual precautions with regard to charge C185000800014 collection have not been carefully observed since the C185000800015 main emphasis in this experiment was on energy C185000800016 spectra. In those cases where the continuous spectra C185000800017 are well described by the four-body shape, the C185000800018 breakup cross section is accurate to within 25 %. C185000800019 STATUS (CURVE) Fig. 3, page 123. C185000800020 ENDBIB 18 0 C185000800021 COMMON 2 3 C185000800022 EN ANG C185000800023 MEV ADEG C185000800024 16.0 30.0 C185000800025 ENDCOMMON 3 0 C185000800026 DATA 3 78 C185000800027 E-CM DATA-CM DATA-ERR C185000800028 MEV MB/SR/MEV MB/SR/MEV C185000800029 1.894 8.781E+00 4.746E-01 C185000800030 1.937 9.357E+00 5.757E-01 C185000800031 1.987 9.507E+00 7.255E-01 C185000800032 2.072 9.065E+00 5.578E-01 C185000800033 2.123 9.283E+00 8.435E-01 C185000800034 2.157 8.440E+00 5.819E-01 C185000800035 2.199 8.440E+00 5.193E-01 C185000800036 2.250 8.440E+00 6.440E-01 C185000800037 2.292 8.440E+00 5.193E-01 C185000800038 2.368 8.373E+00 5.152E-01 C185000800039 2.444 7.552E+00 4.647E-01 C185000800040 2.495 7.316E+00 4.502E-01 C185000800041 2.537 6.651E+00 4.093E-01 C185000800042 2.580 6.292E+00 4.801E-01 C185000800043 2.597 5.812E+00 3.576E-01 C185000800044 2.647 5.675E+00 3.067E-01 C185000800045 2.681 6.443E+00 2.997E-01 C185000800046 2.698 6.047E+00 2.813E-01 C185000800047 2.732 5.242E+00 3.225E-01 C185000800048 2.791 5.242E+00 3.225E-01 C185000800049 2.859 4.998E+00 3.075E-01 C185000800050 2.918 4.766E+00 4.330E-01 C185000800051 2.952 4.617E+00 2.841E-01 C185000800052 2.994 4.617E+00 3.523E-01 C185000800053 3.045 4.728E+00 3.260E-01 C185000800054 3.079 4.544E+00 2.796E-01 C185000800055 3.087 3.908E+00 2.112E-01 C185000800056 3.130 4.098E+00 2.826E-01 C185000800057 3.181 4.066E+00 3.400E-01 C185000800058 3.248 4.034E+00 1.876E-01 C185000800059 3.274 4.919E+00 3.392E-01 C185000800060 3.316 6.047E+00 4.169E-01 C185000800061 3.341 7.087E+00 6.440E-01 C185000800062 3.401 7.433E+00 4.574E-01 C185000800063 3.451 7.433E+00 3.457E-01 C185000800064 3.468 5.497E+00 3.791E-01 C185000800065 3.502 4.333E+00 3.306E-01 C185000800066 3.544 3.414E+00 2.855E-01 C185000800067 3.587 2.486E+00 1.714E-01 C185000800068 3.604 2.296E+00 8.934E-02 C185000800069 3.646 1.824E+00 1.257E-01 C185000800070 3.688 1.685E+00 1.409E-01 C185000800071 3.714 1.619E+00 1.236E-01 C185000800072 3.764 1.556E+00 1.301E-01 C185000800073 3.798 1.349E+00 8.299E-02 C185000800074 3.832 1.472E+00 7.956E-02 C185000800075 3.866 1.403E+00 9.677E-02 C185000800076 3.934 1.286E+00 1.075E-01 C185000800077 4.010 1.055E+00 8.048E-02 C185000800078 4.086 1.046E+00 6.438E-02 C185000800079 4.162 1.055E+00 1.331E-01 C185000800080 4.196 8.856E-01 7.405E-02 C185000800081 4.238 8.927E-01 6.155E-02 C185000800082 4.289 9.070E-01 6.254E-02 C185000800083 4.357 7.738E-01 5.905E-02 C185000800084 4.399 8.311E-01 8.149E-02 C185000800085 4.416 7.148E-01 7.008E-02 C185000800086 4.475 7.556E-01 7.948E-02 C185000800087 4.560 6.655E-01 5.078E-02 C185000800088 4.585 7.320E-01 5.047E-02 C185000800089 4.619 6.245E-01 6.124E-02 C185000800090 4.653 5.633E-01 4.710E-02 C185000800091 4.695 5.286E-01 5.560E-02 C185000800092 4.755 4.267E-01 2.942E-02 C185000800093 4.805 4.656E-01 3.553E-02 C185000800094 4.848 4.922E-01 3.756E-02 C185000800095 4.890 5.861E-01 C185000800096 4.915 1.685E+00 C185000800097 4.932 3.667E+00 C185000800098 4.983 7.087E+00 C185000800099 5.017 1.005E+01 C185000800100 5.051 1.187E+01 C185000800101 5.085 9.357E+00 C185000800102 5.152 5.812E+00 C185000800103 5.186 2.913E+00 C185000800104 5.229 1.328E+00 C185000800105 5.245 6.396E-01 C185000800106 5.305 2.088E-01 C185000800107 ENDDATA 80 0 C185000800108 ENDSUBENT 107 0 C185000899999 SUBENT C1850009 20180315 C174C185000900001 BIB 5 18 C185000900002 REACTION (6-C-12(P,X)2-HE-4,,DA/DE) C185000900003 SAMPLE A thin self-supported polystyrene (CH) target located C185000900004 at the center of a 1 m diam. scattering chamber. C185000900005 Targets of thicknesses ranging from 50 to C185000900006 150 microg/cm2 were used. C185000900007 DETECTOR (SIBAR) The alpha spectra were measured using a thin C185000900008 Ortec Surface Barrier detector (50 microm thickness, C185000900009 totally depleted at a reverse bias of about 100 V). C185000900010 ERR-ANALYS (DATA-ERR) The absolute differential cross sections C185000900011 for the ground state group are accurate to within C185000900012 about 25%. The large uncertainty is due to the fact C185000900013 that the usual precautions with regard to charge C185000900014 collection have not been carefully observed since the C185000900015 main emphasis in this experiment was on energy C185000900016 spectra. In those cases where the continuous spectra C185000900017 are well described by the four-body shape, the C185000900018 breakup cross section is accurate to within 25 %. C185000900019 STATUS (CURVE) Fig. 3, page 123. C185000900020 ENDBIB 18 0 C185000900021 COMMON 2 3 C185000900022 EN ANG C185000900023 MEV ADEG C185000900024 16.0 60.0 C185000900025 ENDCOMMON 3 0 C185000900026 DATA 3 74 C185000900027 E-CM DATA-CM DATA-ERR C185000900028 MEV MB/SR/MEV MB/SR/MEV C185000900029 1.717 1.019E+01 6.612E-01 C185000900030 1.748 1.039E+01 5.804E-01 C185000900031 1.778 9.262E+00 4.332E-01 C185000900032 1.840 9.174E+00 5.124E-01 C185000900033 1.881 8.914E+00 5.782E-01 C185000900034 1.932 8.100E+00 4.524E-01 C185000900035 1.993 7.870E+00 6.501E-01 C185000900036 2.044 7.946E+00 6.564E-01 C185000900037 2.095 8.178E+00 6.755E-01 C185000900038 2.136 8.022E+00 4.481E-01 C185000900039 2.218 7.721E+00 4.313E-01 C185000900040 2.258 7.431E+00 4.151E-01 C185000900041 2.289 7.016E+00 4.550E-01 C185000900042 2.320 6.687E+00 4.338E-01 C185000900043 2.371 6.752E+00 3.771E-01 C185000900044 2.412 7.083E+00 6.471E-01 C185000900045 2.452 6.624E+00 4.296E-01 C185000900046 2.483 6.882E+00 3.844E-01 C185000900047 2.524 6.752E+00 4.379E-01 C185000900048 2.555 6.498E+00 4.215E-01 C185000900049 2.585 6.194E+00 3.460E-01 C185000900050 2.626 5.904E+00 4.877E-01 C185000900051 2.657 5.469E+00 3.547E-01 C185000900052 2.687 5.114E+00 3.773E-01 C185000900053 2.759 5.469E+00 4.518E-01 C185000900054 2.810 5.213E+00 3.846E-01 C185000900055 2.851 4.782E+00 3.951E-01 C185000900056 2.871 4.345E+00 2.427E-01 C185000900057 2.943 4.429E+00 3.268E-01 C185000900058 3.004 4.647E+00 3.428E-01 C185000900059 3.065 4.782E+00 3.102E-01 C185000900060 3.106 4.304E+00 2.792E-01 C185000900061 3.157 4.472E+00 3.299E-01 C185000900062 3.188 4.142E+00 2.314E-01 C185000900063 3.229 4.603E+00 2.571E-01 C185000900064 3.269 6.019E+00 5.498E-01 C185000900065 3.300 8.416E+00 5.459E-01 C185000900066 3.361 1.133E+01 6.327E-01 C185000900067 3.412 1.235E+01 8.008E-01 C185000900068 3.453 1.122E+01 9.267E-01 C185000900069 3.474 7.946E+00 5.862E-01 C185000900070 3.515 5.065E+00 3.285E-01 C185000900071 3.555 3.229E+00 2.382E-01 C185000900072 3.586 2.422E+00 1.571E-01 C185000900073 3.586 1.888E+00 1.055E-01 C185000900074 3.668 1.651E+00 7.723E-02 C185000900075 3.698 1.417E+00 1.170E-01 C185000900076 3.749 1.300E+00 7.259E-02 C185000900077 3.801 1.083E+00 7.026E-02 C185000900078 3.862 8.608E-01 7.111E-02 C185000900079 3.913 1.023E+00 5.713E-02 C185000900080 3.964 7.600E-01 4.929E-02 C185000900081 3.974 9.030E-01 7.460E-02 C185000900082 4.015 7.314E-01 6.042E-02 C185000900083 4.087 6.906E-01 4.479E-02 C185000900084 4.087 5.487E-01 4.048E-02 C185000900085 4.127 6.215E-01 5.678E-02 C185000900086 4.178 5.435E-01 4.965E-02 C185000900087 4.209 4.753E-01 3.506E-02 C185000900088 4.250 4.402E-01 2.855E-02 C185000900089 4.464 3.887E-01 C185000900090 4.832 7.245E-01 C185000900091 4.853 1.033E+00 C185000900092 4.904 3.198E+00 C185000900093 4.944 8.336E+00 C185000900094 4.995 1.760E+01 C185000900095 5.016 2.657E+01 C185000900096 5.067 2.761E+01 C185000900097 5.118 1.974E+01 C185000900098 5.159 1.029E+01 C185000900099 5.190 3.355E+00 C185000900100 5.230 1.083E+00 C185000900101 5.261 3.887E-01 C185000900102 5.312 1.859E-01 C185000900103 ENDDATA 76 0 C185000900104 ENDSUBENT 103 0 C185000999999 SUBENT C1850010 20180315 C174C185001000001 BIB 5 18 C185001000002 REACTION (6-C-12(P,X)2-HE-4,,DA/DE) C185001000003 SAMPLE A thin self-supported polystyrene (CH) target located C185001000004 at the center of a 1 m diam. scattering chamber. C185001000005 Targets of thicknesses ranging from 50 to C185001000006 150 microg/cm2 were used. C185001000007 DETECTOR (SIBAR) The alpha spectra were measured using a thin C185001000008 Ortec Surface Barrier detector (50 microm thickness, C185001000009 totally depleted at a reverse bias of about 100 V). C185001000010 ERR-ANALYS (DATA-ERR) The absolute differential cross sections C185001000011 for the ground state group are accurate to within C185001000012 about 25%. The large uncertainty is due to the fact C185001000013 that the usual precautions with regard to charge C185001000014 collection have not been carefully observed since the C185001000015 main emphasis in this experiment was on energy C185001000016 spectra. In those cases where the continuous spectra C185001000017 are well described by the four-body shape, the C185001000018 breakup cross section is accurate to within 25 %. C185001000019 STATUS (CURVE) Fig. 3, page 123. C185001000020 ENDBIB 18 0 C185001000021 COMMON 2 3 C185001000022 EN ANG C185001000023 MEV ADEG C185001000024 16.0 90.0 C185001000025 ENDCOMMON 3 0 C185001000026 DATA 3 67 C185001000027 E-CM DATA-CM DATA-ERR C185001000028 MEV MB/SR/MEV MB/SR/MEV C185001000029 2.289 8.752E+00 4.861E-01 C185001000030 2.361 8.587E+00 4.769E-01 C185001000031 2.412 7.659E+00 4.254E-01 C185001000032 2.422 8.345E+00 4.635E-01 C185001000033 2.483 7.587E+00 4.214E-01 C185001000034 2.524 7.098E+00 3.300E-01 C185001000035 2.585 6.640E+00 4.282E-01 C185001000036 2.636 5.594E+00 4.103E-01 C185001000037 2.687 4.990E+00 2.771E-01 C185001000038 2.728 4.990E+00 3.660E-01 C185001000039 2.769 4.624E+00 2.982E-01 C185001000040 2.820 4.409E+00 2.843E-01 C185001000041 2.861 4.536E+00 2.926E-01 C185001000042 2.902 4.409E+00 3.234E-01 C185001000043 2.953 4.367E+00 2.816E-01 C185001000044 3.004 4.451E+00 2.870E-01 C185001000045 3.075 3.575E+00 1.663E-01 C185001000046 3.106 4.047E+00 3.324E-01 C185001000047 3.157 3.858E+00 3.169E-01 C185001000048 3.198 3.714E+00 2.063E-01 C185001000049 3.239 3.933E+00 C185001000050 3.300 5.134E+00 C185001000051 3.310 7.165E+00 C185001000052 3.372 1.019E+01 C185001000053 3.433 1.121E+01 C185001000054 3.464 1.010E+01 C185001000055 3.515 6.767E+00 C185001000056 3.555 3.714E+00 C185001000057 3.607 2.586E+00 C185001000058 3.637 2.019E+00 C185001000059 3.709 1.353E+00 1.112E-01 C185001000060 3.790 1.475E+00 1.082E-01 C185001000061 3.811 1.278E+00 1.050E-01 C185001000062 3.882 1.129E+00 7.284E-02 C185001000063 3.933 1.254E+00 1.139E-01 C185001000064 3.964 1.077E+00 7.900E-02 C185001000065 3.984 1.242E+00 8.012E-02 C185001000066 4.025 1.108E+00 C185001000067 4.076 1.067E+00 C185001000068 4.087 9.247E-01 5.964E-02 C185001000069 4.117 9.698E-01 5.386E-02 C185001000070 4.148 1.129E+00 9.277E-02 C185001000071 4.189 9.791E-01 7.182E-02 C185001000072 4.250 8.407E-01 5.422E-02 C185001000073 4.301 8.987E-01 7.382E-02 C185001000074 4.403 8.093E-01 7.352E-02 C185001000075 4.434 7.016E-01 5.763E-02 C185001000076 4.495 6.563E-01 4.815E-02 C185001000077 4.546 5.855E-01 4.295E-02 C185001000078 4.597 6.024E-01 5.472E-02 C185001000079 4.658 5.911E-01 5.369E-02 C185001000080 4.699 5.636E-01 4.629E-02 C185001000081 4.771 4.748E-01 C185001000082 4.832 4.886E-01 C185001000083 4.842 5.799E-01 C185001000084 4.893 9.885E-01 C185001000085 4.955 2.791E+00 C185001000086 4.975 7.165E+00 C185001000087 5.036 9.905E+00 C185001000088 5.057 1.059E+01 C185001000089 5.108 1.059E+01 C185001000090 5.138 6.832E+00 C185001000091 5.149 2.739E+00 C185001000092 5.179 1.547E+00 C185001000093 5.179 8.734E-01 C185001000094 5.220 5.425E-01 C185001000095 5.261 1.106E-01 C185001000096 ENDDATA 69 0 C185001000097 ENDSUBENT 96 0 C185001099999 SUBENT C1850011 20180315 C174C185001100001 BIB 5 18 C185001100002 REACTION (6-C-12(P,X)2-HE-4,,DA/DE) C185001100003 SAMPLE A thin self-supported polystyrene (CH) target located C185001100004 at the center of a 1 m diam. scattering chamber. C185001100005 Targets of thicknesses ranging from 50 to C185001100006 150 microg/cm2 were used. C185001100007 DETECTOR (SIBAR) The alpha spectra were measured using a thin C185001100008 Ortec Surface Barrier detector (50 microm thickness, C185001100009 totally depleted at a reverse bias of about 100 V). C185001100010 ERR-ANALYS (DATA-ERR) The absolute differential cross sections C185001100011 for the ground state group are accurate to within C185001100012 about 25%. The large uncertainty is due to the fact C185001100013 that the usual precautions with regard to charge C185001100014 collection have not been carefully observed since the C185001100015 main emphasis in this experiment was on energy C185001100016 spectra. In those cases where the continuous spectra C185001100017 are well described by the four-body shape, the C185001100018 breakup cross section is accurate to within 25 %. C185001100019 STATUS (CURVE) Fig. 3, page 123. C185001100020 ENDBIB 18 0 C185001100021 COMMON 2 3 C185001100022 EN ANG C185001100023 MEV ADEG C185001100024 16.0 120.0 C185001100025 ENDCOMMON 3 0 C185001100026 DATA 3 30 C185001100027 E-CM DATA-CM DATA-ERR C185001100028 MEV MB/SR/MEV MB/SR/MEV C185001100029 3.617 1.699E+00 1.248E-01 C185001100030 3.729 1.377E+00 7.662E-02 C185001100031 3.770 1.217E+00 6.769E-02 C185001100032 3.801 9.313E-01 6.017E-02 C185001100033 3.913 1.025E+00 4.773E-02 C185001100034 3.964 7.695E-01 5.655E-02 C185001100035 4.087 5.458E-01 4.011E-02 C185001100036 4.127 7.478E-01 4.831E-02 C185001100037 4.158 5.725E-01 3.185E-02 C185001100038 4.219 5.947E-01 3.309E-02 C185001100039 4.291 4.961E-01 3.205E-02 C185001100040 4.342 5.406E-01 3.973E-02 C185001100041 4.424 5.105E-01 3.752E-02 C185001100042 4.464 3.871E-01 2.154E-02 C185001100043 4.505 4.022E-01 2.598E-02 C185001100044 4.546 4.553E-01 4.143E-02 C185001100045 4.638 4.259E-01 3.876E-02 C185001100046 4.669 2.908E-01 2.137E-02 C185001100047 4.720 2.936E-01 1.897E-02 C185001100048 4.791 2.936E-01 1.897E-02 C185001100049 4.832 4.685E-01 C185001100050 4.893 1.748E+00 C185001100051 5.016 7.107E+00 C185001100052 5.057 7.314E+00 C185001100053 5.098 6.973E+00 C185001100054 5.128 3.576E+00 C185001100055 5.159 1.288E+00 C185001100056 5.200 3.726E-01 C185001100057 5.261 2.643E-01 C185001100058 5.292 1.688E-01 C185001100059 ENDDATA 32 0 C185001100060 ENDSUBENT 59 0 C185001199999 SUBENT C1850012 20180315 C174C185001200001 BIB 5 18 C185001200002 REACTION (6-C-12(P,X)2-HE-4,,DA/DE) C185001200003 SAMPLE A thin self-supported polystyrene (CH) target located C185001200004 at the center of a 1 m diam. scattering chamber. C185001200005 Targets of thicknesses ranging from 50 to C185001200006 150 microg/cm2 were used. C185001200007 DETECTOR (SIBAR) The alpha spectra were measured using a thin C185001200008 Ortec Surface Barrier detector (50 microm thickness, C185001200009 totally depleted at a reverse bias of about 100 V). C185001200010 ERR-ANALYS (DATA-ERR) The absolute differential cross sections C185001200011 for the ground state group are accurate to within C185001200012 about 25%. The large uncertainty is due to the fact C185001200013 that the usual precautions with regard to charge C185001200014 collection have not been carefully observed since the C185001200015 main emphasis in this experiment was on energy C185001200016 spectra. In those cases where the continuous spectra C185001200017 are well described by the four-body shape, the C185001200018 breakup cross section is accurate to within 25 %. C185001200019 STATUS (CURVE) Fig. 4, page 123. C185001200020 ENDBIB 18 0 C185001200021 COMMON 2 3 C185001200022 EN ANG C185001200023 MEV ADEG C185001200024 12.7 22.0 C185001200025 ENDCOMMON 3 0 C185001200026 DATA 3 53 C185001200027 E-CM DATA-CM DATA-ERR C185001200028 MEV MB/SR/MEV MB/SR/MEV C185001200029 1.105 1.031E+01 5.151E-01 C185001200030 1.150 1.014E+01 5.882E-01 C185001200031 1.182 9.385E+00 4.689E-01 C185001200032 1.214 9.306E+00 4.649E-01 C185001200033 1.241 8.917E+00 5.175E-01 C185001200034 1.282 8.257E+00 4.125E-01 C185001200035 1.309 7.452E+00 3.116E-01 C185001200036 1.354 7.516E+00 4.362E-01 C185001200037 1.395 7.141E+00 4.144E-01 C185001200038 1.413 6.726E+00 4.443E-01 C185001200039 1.449 6.726E+00 4.977E-01 C185001200040 1.508 6.726E+00 3.904E-01 C185001200041 1.535 6.669E+00 4.405E-01 C185001200042 1.567 6.123E+00 4.531E-01 C185001200043 1.608 6.123E+00 3.554E-01 C185001200044 1.631 6.019E+00 4.454E-01 C185001200045 1.676 5.918E+00 3.434E-01 C185001200046 1.708 6.071E+00 3.524E-01 C185001200047 1.758 5.867E+00 3.405E-01 C185001200048 1.785 5.867E+00 3.405E-01 C185001200049 1.808 5.622E+00 2.809E-01 C185001200050 1.862 6.019E+00 3.007E-01 C185001200051 1.898 5.768E+00 2.881E-01 C185001200052 1.921 5.387E+00 2.691E-01 C185001200053 1.957 5.206E+00 3.438E-01 C185001200054 1.993 5.118E+00 2.970E-01 C185001200055 2.039 4.862E+00 2.429E-01 C185001200056 2.075 4.739E+00 2.368E-01 C185001200057 2.098 4.464E+00 1.499E-01 C185001200058 2.143 3.828E+00 2.528E-01 C185001200059 2.188 3.426E+00 1.988E-01 C185001200060 2.225 2.767E+00 1.606E-01 C185001200061 2.261 2.476E+00 1.635E-01 C185001200062 2.284 1.949E+00 1.596E-01 C185001200063 2.324 1.672E+00 1.237E-01 C185001200064 2.370 1.588E+00 1.175E-01 C185001200065 2.415 1.362E+00 C185001200066 2.447 1.119E+00 C185001200067 2.569 7.951E-01 C185001200068 2.606 7.115E-01 C185001200069 2.633 6.206E-01 C185001200070 2.664 5.896E-01 C185001200071 2.683 5.367E-01 C185001200072 2.705 5.896E-01 C185001200073 2.755 2.105E+00 C185001200074 2.800 1.076E+01 C185001200075 2.837 3.211E+01 C185001200076 2.868 4.184E+01 C185001200077 2.927 2.730E+01 C185001200078 2.964 8.117E+00 C185001200079 2.973 1.339E+00 C185001200080 3.023 1.845E-01 C185001200081 3.068 9.318E-02 C185001200082 ENDDATA 55 0 C185001200083 ENDSUBENT 82 0 C185001299999 SUBENT C1850013 20180315 C174C185001300001 BIB 5 18 C185001300002 REACTION (6-C-12(P,X)2-HE-4,,DA/DE) C185001300003 SAMPLE A thin self-supported polystyrene (CH) target located C185001300004 at the center of a 1 m diam. scattering chamber. C185001300005 Targets of thicknesses ranging from 50 to C185001300006 150 microg/cm2 were used. C185001300007 DETECTOR (SIBAR) The alpha spectra were measured using a thin C185001300008 Ortec Surface Barrier detector (50 microm thickness, C185001300009 totally depleted at a reverse bias of about 100 V). C185001300010 ERR-ANALYS (DATA-ERR) The absolute differential cross sections C185001300011 for the ground state group are accurate to within C185001300012 about 25%. The large uncertainty is due to the fact C185001300013 that the usual precautions with regard to charge C185001300014 collection have not been carefully observed since the C185001300015 main emphasis in this experiment was on energy C185001300016 spectra. In those cases where the continuous spectra C185001300017 are well described by the four-body shape, the C185001300018 breakup cross section is accurate to within 25 %. C185001300019 STATUS (CURVE) Fig. 4, page 123. C185001300020 ENDBIB 18 0 C185001300021 COMMON 2 3 C185001300022 EN ANG C185001300023 MEV ADEG C185001300024 12.7 30.0 C185001300025 ENDCOMMON 3 0 C185001300026 DATA 3 51 C185001300027 E-CM DATA-CM DATA-ERR C185001300028 MEV MB/SR/MEV MB/SR/MEV C185001300029 1.159 7.411E+00 3.105E-01 C185001300030 1.182 6.518E+00 3.263E-01 C185001300031 1.223 6.245E+00 3.127E-01 C185001300032 1.259 6.462E+00 3.236E-01 C185001300033 1.295 6.298E+00 3.664E-01 C185001300034 1.318 5.635E+00 3.730E-01 C185001300035 1.363 5.684E+00 2.846E-01 C185001300036 1.390 5.173E+00 3.424E-01 C185001300037 1.422 5.353E+00 2.680E-01 C185001300038 1.454 5.217E+00 2.612E-01 C185001300039 1.504 5.307E+00 2.224E-01 C185001300040 1.535 5.262E+00 3.483E-01 C185001300041 1.563 5.129E+00 2.568E-01 C185001300042 1.599 5.173E+00 2.590E-01 C185001300043 1.640 5.217E+00 3.453E-01 C185001300044 1.676 4.999E+00 2.503E-01 C185001300045 1.712 5.042E+00 2.932E-01 C185001300046 1.753 5.042E+00 2.524E-01 C185001300047 1.794 5.307E+00 3.087E-01 C185001300048 1.826 4.668E+00 2.337E-01 C185001300049 1.866 4.748E+00 2.762E-01 C185001300050 1.912 4.285E+00 2.492E-01 C185001300051 1.953 4.472E+00 3.316E-01 C185001300052 1.980 3.833E+00 2.230E-01 C185001300053 2.057 3.642E+00 2.118E-01 C185001300054 2.089 3.258E+00 2.416E-01 C185001300055 2.129 2.793E+00 2.291E-01 C185001300056 2.170 2.520E+00 1.668E-01 C185001300057 2.207 2.373E+00 1.760E-01 C185001300058 2.234 2.142E+00 1.418E-01 C185001300059 2.275 1.685E+00 1.116E-01 C185001300060 2.311 1.587E+00 9.232E-02 C185001300061 2.356 1.292E+00 8.555E-02 C185001300062 2.406 1.217E+00 8.058E-02 C185001300063 2.451 1.052E+00 8.635E-02 C185001300064 2.479 9.256E-01 7.594E-02 C185001300065 2.528 7.866E-01 6.454E-02 C185001300066 2.565 7.038E-01 6.871E-02 C185001300067 2.601 6.033E-01 4.474E-02 C185001300068 2.615 5.491E-01 3.194E-02 C185001300069 2.674 5.127E-01 2.567E-02 C185001300070 2.696 4.666E-01 3.089E-02 C185001300071 2.755 7.409E-01 C185001300072 2.787 4.212E+00 C185001300073 2.805 1.686E+01 C185001300074 2.850 3.149E+01 C185001300075 2.900 3.017E+01 C185001300076 2.923 1.521E+01 C185001300077 2.955 4.141E+00 C185001300078 2.991 6.460E-01 C185001300079 3.023 9.741E-02 C185001300080 ENDDATA 53 0 C185001300081 ENDSUBENT 80 0 C185001399999 SUBENT C1850014 20180315 C174C185001400001 BIB 5 18 C185001400002 REACTION (6-C-12(P,X)2-HE-4,,DA/DE) C185001400003 SAMPLE A thin self-supported polystyrene (CH) target located C185001400004 at the center of a 1 m diam. scattering chamber. C185001400005 Targets of thicknesses ranging from 50 to C185001400006 150 microg/cm2 were used. C185001400007 DETECTOR (SIBAR) The alpha spectra were measured using a thin C185001400008 Ortec Surface Barrier detector (50 microm thickness, C185001400009 totally depleted at a reverse bias of about 100 V). C185001400010 ERR-ANALYS (DATA-ERR) The absolute differential cross sections C185001400011 for the ground state group are accurate to within C185001400012 about 25%. The large uncertainty is due to the fact C185001400013 that the usual precautions with regard to charge C185001400014 collection have not been carefully observed since the C185001400015 main emphasis in this experiment was on energy C185001400016 spectra. In those cases where the continuous spectra C185001400017 are well described by the four-body shape, the C185001400018 breakup cross section is accurate to within 25 %. C185001400019 STATUS (CURVE) Fig. 4, page 123. C185001400020 ENDBIB 18 0 C185001400021 COMMON 2 3 C185001400022 EN ANG C185001400023 MEV ADEG C185001400024 12.7 45.0 C185001400025 ENDCOMMON 3 0 C185001400026 DATA 3 41 C185001400027 E-CM DATA-CM DATA-ERR C185001400028 MEV MB/SR/MEV MB/SR/MEV C185001400029 1.413 7.273E+00 3.660E-01 C185001400030 1.427 5.865E+00 2.952E-01 C185001400031 1.467 5.428E+00 3.611E-01 C185001400032 1.508 5.110E+00 4.214E-01 C185001400033 1.545 5.289E+00 3.093E-01 C185001400034 1.585 5.428E+00 3.173E-01 C185001400035 1.622 4.937E+00 3.680E-01 C185001400036 1.658 5.199E+00 3.040E-01 C185001400037 1.699 4.980E+00 4.107E-01 C185001400038 1.726 4.649E+00 3.834E-01 C185001400039 1.771 4.491E+00 3.348E-01 C185001400040 1.798 4.812E+00 3.201E-01 C185001400041 1.862 4.609E+00 3.435E-01 C185001400042 1.894 4.339E+00 3.234E-01 C185001400043 1.916 4.051E+00 2.368E-01 C185001400044 1.962 4.051E+00 2.695E-01 C185001400045 2.012 3.685E+00 2.746E-01 C185001400046 2.057 3.469E+00 2.586E-01 C185001400047 2.089 2.774E+00 2.067E-01 C185001400048 2.111 2.921E+00 1.943E-01 C185001400049 2.152 2.438E+00 1.622E-01 C185001400050 2.202 2.143E+00 1.597E-01 C185001400051 2.247 2.052E+00 1.692E-01 C185001400052 2.284 1.899E+00 1.566E-01 C185001400053 2.315 1.655E+00 1.495E-01 C185001400054 2.374 1.417E+00 1.169E-01 C185001400055 2.401 1.246E+00 8.289E-02 C185001400056 2.447 1.204E+00 8.009E-02 C185001400057 2.483 1.204E+00 8.009E-02 C185001400058 2.519 9.060E-01 6.753E-02 C185001400059 2.560 7.059E-01 4.697E-02 C185001400060 2.606 7.306E-01 4.861E-02 C185001400061 2.633 5.547E-01 4.575E-02 C185001400062 2.696 5.178E-01 3.860E-02 C185001400063 2.732 5.841E-01 C185001400064 2.746 1.031E+00 C185001400065 2.805 4.121E+00 C185001400066 2.868 1.460E+01 C185001400067 2.914 1.229E+01 C185001400068 2.950 3.847E+00 C185001400069 2.991 5.841E-01 C185001400070 ENDDATA 43 0 C185001400071 ENDSUBENT 70 0 C185001499999 SUBENT C1850015 20180315 C174C185001500001 BIB 5 18 C185001500002 REACTION (6-C-12(P,A)5-B-9,,DA/DE) C185001500003 SAMPLE A thin self-supported polystyrene (CH) target located C185001500004 at the center of a 1 m diam. scattering chamber. C185001500005 Targets of thicknesses ranging from 50 to C185001500006 150 microg/cm2 were used. C185001500007 DETECTOR (SIBAR) The alpha spectra were measured using a thin C185001500008 Ortec Surface Barrier detector (50 microm thickness, C185001500009 totally depleted at a reverse bias of about 100 V). C185001500010 ERR-ANALYS (DATA-ERR) The absolute differential cross sections C185001500011 for the ground state group are accurate to within C185001500012 about 25%. The large uncertainty is due to the fact C185001500013 that the usual precautions with regard to charge C185001500014 collection have not been carefully observed since the C185001500015 main emphasis in this experiment was on energy C185001500016 spectra. In those cases where the continuous spectra C185001500017 are well described by the four-body shape, the C185001500018 breakup cross section is accurate to within 25 %. C185001500019 STATUS (CURVE) Fig. 4, page 123. C185001500020 ENDBIB 18 0 C185001500021 COMMON 2 3 C185001500022 EN ANG C185001500023 MEV ADEG C185001500024 12.7 60.0 C185001500025 ENDCOMMON 3 0 C185001500026 DATA 3 30 C185001500027 E-CM DATA-CM DATA-ERR C185001500028 MEV MB/SR/MEV MB/SR/MEV C185001500029 1.784 3.106E+00 2.285E-01 C185001500030 1.829 2.902E+00 1.676E-01 C185001500031 1.884 2.429E+00 1.789E-01 C185001500032 1.911 2.328E+00 1.345E-01 C185001500033 1.957 2.289E+00 1.324E-01 C185001500034 1.984 2.213E+00 1.101E-01 C185001500035 2.043 1.999E+00 1.154E-01 C185001500036 2.084 1.950E+00 1.589E-01 C185001500037 2.121 1.485E+00 4.963E-02 C185001500038 2.162 1.564E+00 1.028E-01 C185001500039 2.207 1.331E+00 9.794E-02 C185001500040 2.248 1.233E+00 9.089E-02 C185001500041 2.298 1.223E+00 9.008E-02 C185001500042 2.353 1.023E+00 7.541E-02 C185001500043 2.389 9.088E-01 3.783E-02 C185001500044 2.430 8.565E-01 4.947E-02 C185001500045 2.462 8.281E-01 6.096E-02 C185001500046 2.508 6.364E-01 5.186E-02 C185001500047 2.540 6.642E-01 3.834E-02 C185001500048 2.604 5.372E-01 2.671E-02 C185001500049 2.640 4.381E-01 5.573E-02 C185001500050 2.677 3.957E-01 1.967E-02 C185001500051 2.739 7.429E-01 C185001500052 2.773 2.465E+00 C185001500053 2.803 6.391E+00 C185001500054 2.842 1.029E+01 C185001500055 2.883 1.004E+01 C185001500056 2.925 6.026E+00 C185001500057 2.959 2.642E+00 C185001500058 3.006 7.635E-01 C185001500059 ENDDATA 32 0 C185001500060 ENDSUBENT 59 0 C185001599999 SUBENT C1850016 20180315 C174C185001600001 BIB 7 24 C185001600002 REACTION (4-BE-9(P,X)0-NN-1,,DA/DE) C185001600003 SAMPLE A 1.28 mg/cm2 Be target evaporated on a 0.5 mm thick C185001600004 tantalum plate which was thick enough to stop the C185001600005 proton beam. C185001600006 DETECTOR (SCIN) The neutron detectors, consisting of 5 x 5 cm C185001600007 plastic scintillators mounted on RCA-6655 C185001600008 photomultipliers, were positioned, at 15 degree C185001600009 angular intervals in a well collimated and shielded C185001600010 geometry. C185001600011 METHOD (TOF) The neutron spectra were observed using time-of- C185001600012 flight techniques. A flight-path of about 10 m was C185001600013 chosen as an optimum considering neutron intensities C185001600014 and resolution of the experimental equipment. C185001600015 REL-REF (M,,J.D.Anderson+,J,NIM,15,178,1962) C185001600016 ERR-ANALYS (DATA-ERR) The absolute differential cross sections C185001600017 for the ground state group are accurate to within C185001600018 about 25%. The large uncertainty is due to the fact C185001600019 that the usual precautions with regard to charge C185001600020 collection have not been carefully observed since the C185001600021 main emphasis in this experiment was on energy C185001600022 spectra. In those cases where the continuous spectra C185001600023 are well described by the four-body shape, the C185001600024 breakup cross section is accurate to within 25 %. C185001600025 STATUS (CURVE) Fig. 5, page 125. C185001600026 ENDBIB 24 0 C185001600027 COMMON 2 3 C185001600028 EN ANG C185001600029 MEV ADEG C185001600030 7.4 15.0 C185001600031 ENDCOMMON 3 0 C185001600032 DATA 3 94 C185001600033 E-CM DATA-CM DATA-ERR C185001600034 MEV MB/SR/MEV MB/SR/MEV C185001600035 0.100 1.545E+00 C185001600036 0.162 1.774E+00 C185001600037 0.189 2.037E+00 C185001600038 0.268 1.997E+00 C185001600039 0.313 1.882E+00 C185001600040 0.340 1.576E+00 C185001600041 0.411 1.774E+00 C185001600042 0.482 1.845E+00 C185001600043 0.526 1.997E+00 C185001600044 0.588 2.119E+00 C185001600045 0.677 2.037E+00 2.278E-01 C185001600046 0.775 1.774E+00 C185001600047 0.846 1.705E+00 C185001600048 0.873 1.456E+00 C185001600049 0.917 1.345E+00 C185001600050 0.944 1.219E+00 C185001600051 0.980 1.040E+00 C185001600052 1.042 1.020E+00 C185001600053 1.086 1.171E+00 C185001600054 1.104 6.474E-01 2.524E-01 C185001600055 1.157 9.804E-01 C185001600056 1.184 1.148E+00 C185001600057 1.228 1.268E+00 C185001600058 1.264 1.427E+00 C185001600059 1.299 1.920E+00 C185001600060 1.388 4.581E+00 C185001600061 1.424 8.794E+00 C185001600062 1.477 1.137E+01 1.272E+00 C185001600063 1.531 1.010E+01 C185001600064 1.628 2.907E+00 C185001600065 1.682 1.082E+00 C185001600066 1.753 4.536E-01 C185001600067 1.779 2.660E-01 C185001600068 1.842 2.227E-01 4.351E-02 C185001600069 1.957 2.017E-01 C185001600070 1.993 2.227E-01 C185001600071 2.073 2.057E-01 C185001600072 2.126 1.500E-01 C185001600073 2.179 1.623E-01 C185001600074 2.215 1.864E-01 C185001600075 2.268 1.530E-01 C185001600076 2.304 1.623E-01 C185001600077 2.366 1.591E-01 C185001600078 2.455 1.386E-01 C185001600079 2.562 1.207E-01 1.559E-02 C185001600080 2.579 8.970E-02 C185001600081 2.624 1.137E-01 C185001600082 2.650 8.970E-02 C185001600083 2.659 7.076E-02 C185001600084 2.722 6.802E-02 C185001600085 2.722 8.622E-02 C185001600086 2.775 1.051E-01 C185001600087 2.810 7.361E-02 C185001600088 2.873 6.285E-02 C185001600089 2.899 5.057E-02 C185001600090 2.926 6.938E-02 C185001600091 2.970 4.317E-02 C185001600092 2.988 5.693E-02 C185001600093 3.024 6.938E-02 C185001600094 3.059 4.317E-02 C185001600095 3.148 6.938E-02 C185001600096 3.166 3.474E-02 5.661E-03 C185001600097 3.219 2.740E-02 C185001600098 3.237 3.339E-02 C185001600099 3.299 3.989E-02 C185001600100 3.326 5.693E-02 C185001600101 3.353 3.543E-02 C185001600102 3.379 3.147E-02 C185001600103 3.406 2.294E-02 C185001600104 3.450 1.639E-02 C185001600105 3.468 4.233E-02 C185001600106 3.557 2.795E-02 C185001600107 3.566 1.882E-02 C185001600108 3.601 3.274E-02 C185001600109 3.619 5.261E-02 C185001600110 3.681 3.989E-02 C185001600111 3.726 7.217E-02 C185001600112 3.744 1.280E-01 2.296E-02 C185001600113 3.770 2.057E-01 C185001600114 3.832 3.722E-01 C185001600115 3.841 5.637E-01 C185001600116 3.912 8.046E-01 C185001600117 3.939 1.809E+00 C185001600118 4.019 2.851E+00 C185001600119 4.099 3.209E+00 3.589E-01 C185001600120 4.161 3.085E+00 C185001600121 4.232 2.294E+00 C185001600122 4.277 2.037E+00 C185001600123 4.312 1.195E+00 C185001600124 4.463 1.978E-01 C185001600125 4.508 6.041E-02 C185001600126 4.570 1.485E-02 C185001600127 4.606 3.440E-03 C185001600128 4.650 8.126E-04 C185001600129 ENDDATA 96 0 C185001600130 ENDSUBENT 129 0 C185001699999 SUBENT C1850017 20180315 C174C185001700001 BIB 7 24 C185001700002 REACTION (4-BE-9(P,X)0-NN-1,,DA/DE) C185001700003 SAMPLE A 1.28 mg/cm2 Be target evaporated on a 0.5 mm thick C185001700004 tantalum plate which was thick enough to stop the C185001700005 proton beam. C185001700006 DETECTOR (SCIN) The neutron detectors, consisting of 5 x 5 cm C185001700007 plastic scintillators mounted on RCA-6655 C185001700008 photomultipliers, were positioned, at 15 degree C185001700009 angular intervals in a well collimated and shielded C185001700010 geometry. C185001700011 METHOD (TOF) The neutron spectra were observed using time-of- C185001700012 flight techniques. A flight-path of about 10 m was C185001700013 chosen as an optimum considering neutron intensities C185001700014 and resolution of the experimental equipment. C185001700015 REL-REF (M,,J.D.Anderson+,J,NIM,15,178,1962) C185001700016 ERR-ANALYS (DATA-ERR) The absolute differential cross sections C185001700017 for the ground state group are accurate to within C185001700018 about 25%. The large uncertainty is due to the fact C185001700019 that the usual precautions with regard to charge C185001700020 collection have not been carefully observed since the C185001700021 main emphasis in this experiment was on energy C185001700022 spectra. In those cases where the continuous spectra C185001700023 are well described by the four-body shape, the C185001700024 breakup cross section is accurate to within 25 %. C185001700025 STATUS (CURVE) Fig. 5, page 125. C185001700026 ENDBIB 24 0 C185001700027 COMMON 2 3 C185001700028 EN ANG C185001700029 MEV ADEG C185001700030 7.4 45.0 C185001700031 ENDCOMMON 3 0 C185001700032 DATA 3 69 C185001700033 E-CM DATA-CM DATA-ERR C185001700034 MEV MB/SR/MEV MB/SR/MEV C185001700035 0.473 1.174E+01 C185001700036 0.517 1.068E+01 C185001700037 0.580 1.058E+01 C185001700038 0.677 9.099E+00 4.198E-01 C185001700039 0.748 9.449E+00 C185001700040 0.793 8.761E+00 C185001700041 0.864 8.597E+00 C185001700042 0.900 8.928E+00 C185001700043 1.006 9.013E+00 C185001700044 1.086 8.436E+00 C185001700045 1.113 9.360E+00 C185001700046 1.211 9.360E+00 C185001700047 1.291 1.109E+01 C185001700048 1.379 1.392E+01 C185001700049 1.415 1.730E+01 C185001700050 1.451 2.253E+01 C185001700051 1.531 2.524E+01 1.391E+00 C185001700052 1.584 1.848E+01 C185001700053 1.628 1.099E+01 C185001700054 1.691 7.050E+00 C185001700055 1.726 5.620E+00 C185001700056 1.779 4.697E+00 C185001700057 1.842 4.653E+00 C185001700058 1.957 4.038E+00 2.939E-01 C185001700059 2.019 3.815E+00 C185001700060 2.090 4.273E+00 C185001700061 2.126 3.744E+00 C185001700062 2.250 3.504E+00 C185001700063 2.313 3.407E+00 C185001700064 2.348 3.249E+00 C185001700065 2.384 2.874E+00 C185001700066 2.464 3.311E+00 C185001700067 2.570 3.129E+00 C185001700068 2.633 2.957E+00 C185001700069 2.704 2.901E+00 C185001700070 2.775 2.045E+00 C185001700071 2.935 2.313E+00 C185001700072 2.953 1.585E+00 C185001700073 3.041 2.379E+00 C185001700074 3.041 2.185E+00 C185001700075 3.077 1.541E+00 C185001700076 3.175 1.470E+00 3.415E-01 C185001700077 3.219 2.227E+00 C185001700078 3.246 1.759E+00 C185001700079 3.255 1.631E+00 C185001700080 3.308 1.600E+00 C185001700081 3.344 1.933E+00 C185001700082 3.344 1.709E+00 C185001700083 3.406 2.448E+00 C185001700084 3.406 1.662E+00 C185001700085 3.495 2.379E+00 C185001700086 3.601 2.165E+00 C185001700087 3.690 3.571E+00 C185001700088 3.850 7.532E+00 C185001700089 3.859 9.185E+00 C185001700090 3.921 1.120E+01 C185001700091 3.975 1.634E+01 1.046E+00 C185001700092 4.001 1.901E+01 C185001700093 4.144 2.211E+01 C185001700094 4.250 1.619E+01 C185001700095 4.304 1.163E+01 C185001700096 4.321 7.676E+00 C185001700097 4.375 4.971E+00 C185001700098 4.410 3.639E+00 C185001700099 4.455 2.402E+00 C185001700100 4.499 1.171E+00 C185001700101 4.543 6.400E-01 C185001700102 4.570 4.428E-01 C185001700103 4.659 2.840E-01 C185001700104 ENDDATA 71 0 C185001700105 ENDSUBENT 104 0 C185001799999 SUBENT C1850018 20180315 C174C185001800001 BIB 7 24 C185001800002 REACTION (4-BE-9(P,X)0-NN-1,,DA/DE) C185001800003 SAMPLE A 1.28 mg/cm2 Be target evaporated on a 0.5 mm thick C185001800004 tantalum plate which was thick enough to stop the C185001800005 proton beam. C185001800006 DETECTOR (SCIN) The neutron detectors, consisting of 5 x 5 cm C185001800007 plastic scintillators mounted on RCA-6655 C185001800008 photomultipliers, were positioned, at 15 degree C185001800009 angular intervals in a well collimated and shielded C185001800010 geometry. C185001800011 METHOD (TOF) The neutron spectra were observed using time-of- C185001800012 flight techniques. A flight-path of about 10 m was C185001800013 chosen as an optimum considering neutron intensities C185001800014 and resolution of the experimental equipment. C185001800015 REL-REF (M,,J.D.Anderson+,J,NIM,15,178,1962) C185001800016 ERR-ANALYS (DATA-ERR) The absolute differential cross sections C185001800017 for the ground state group are accurate to within C185001800018 about 25%. The large uncertainty is due to the fact C185001800019 that the usual precautions with regard to charge C185001800020 collection have not been carefully observed since the C185001800021 main emphasis in this experiment was on energy C185001800022 spectra. In those cases where the continuous spectra C185001800023 are well described by the four-body shape, the C185001800024 breakup cross section is accurate to within 25 %. C185001800025 STATUS (CURVE) Fig. 5, page 125. C185001800026 ENDBIB 24 0 C185001800027 COMMON 2 3 C185001800028 EN ANG C185001800029 MEV ADEG C185001800030 7.4 75.0 C185001800031 ENDCOMMON 3 0 C185001800032 DATA 3 64 C185001800033 E-CM DATA-CM DATA-ERR C185001800034 MEV MB/SR/MEV MB/SR/MEV C185001800035 0.864 8.051E+00 6.831E-01 C185001800036 0.997 7.816E+00 C185001800037 1.059 7.296E+00 C185001800038 1.104 7.664E+00 C185001800039 1.166 7.368E+00 C185001800040 1.246 7.664E+00 C185001800041 1.291 8.131E+00 C185001800042 1.371 8.051E+00 C185001800043 1.433 1.384E+01 C185001800044 1.504 2.356E+01 C185001800045 1.539 2.956E+01 C185001800046 1.593 1.824E+01 C185001800047 1.655 8.972E+00 C185001800048 1.726 5.703E+00 C185001800049 1.771 3.661E+00 C185001800050 1.851 3.733E+00 C185001800051 1.957 3.383E+00 4.934E-01 C185001800052 2.010 2.542E+00 C185001800053 2.055 2.697E+00 C185001800054 2.144 2.619E+00 C185001800055 2.259 2.193E+00 C185001800056 2.313 1.783E+00 C185001800057 2.384 1.783E+00 C185001800058 2.437 1.731E+00 C185001800059 2.499 1.422E+00 C185001800060 2.553 1.340E+00 C185001800061 2.730 1.133E+00 C185001800062 2.855 9.126E-01 C185001800063 2.890 9.972E-01 C185001800064 2.961 9.307E-01 C185001800065 3.041 7.347E-01 C185001800066 3.086 8.517E-01 C185001800067 3.193 8.517E-01 C185001800068 3.290 8.351E-01 C185001800069 3.344 5.916E-01 C185001800070 3.406 7.063E-01 C185001800071 3.539 2.560E-01 C185001800072 3.575 5.858E-01 C185001800073 3.584 7.718E-01 C185001800074 3.619 4.858E-01 C185001800075 3.637 3.650E-01 C185001800076 3.681 8.108E-01 C185001800077 3.690 6.338E-01 C185001800078 3.779 1.027E+00 2.001E-01 C185001800079 3.815 7.718E-01 C185001800080 3.895 1.464E+00 C185001800081 3.930 2.150E+00 C185001800082 3.948 3.252E+00 C185001800083 3.984 4.637E+00 C185001800084 4.046 9.426E+00 C185001800085 4.072 1.589E+01 C185001800086 4.081 2.033E+01 C185001800087 4.135 2.310E+01 C185001800088 4.152 2.841E+01 1.631E+00 C185001800089 4.241 2.813E+01 C185001800090 4.295 1.702E+01 C185001800091 4.321 1.230E+01 C185001800092 4.357 6.050E+00 C185001800093 4.455 2.976E+00 C185001800094 4.508 8.517E-01 C185001800095 4.552 9.972E-01 C185001800096 4.579 7.420E-01 C185001800097 4.650 8.188E-01 C185001800098 4.677 5.743E-01 C185001800099 ENDDATA 66 0 C185001800100 ENDSUBENT 99 0 C185001899999 SUBENT C1850019 20180315 C174C185001900001 BIB 7 24 C185001900002 REACTION (4-BE-9(P,X)0-NN-1,,DA/DE) C185001900003 SAMPLE A 1.28 mg/cm2 Be target evaporated on a 0.5 mm thick C185001900004 tantalum plate which was thick enough to stop the C185001900005 proton beam. C185001900006 DETECTOR (SCIN) The neutron detectors, consisting of 5 x 5 cm C185001900007 plastic scintillators mounted on RCA-6655 C185001900008 photomultipliers, were positioned, at 15 degree C185001900009 angular intervals in a well collimated and shielded C185001900010 geometry. C185001900011 METHOD (TOF) The neutron spectra were observed using time-of- C185001900012 flight techniques. A flight-path of about 10 m was C185001900013 chosen as an optimum considering neutron intensities C185001900014 and resolution of the experimental equipment. C185001900015 REL-REF (M,,J.D.Anderson+,J,NIM,15,178,1962) C185001900016 ERR-ANALYS (DATA-ERR) The absolute differential cross sections C185001900017 for the ground state group are accurate to within C185001900018 about 25%. The large uncertainty is due to the fact C185001900019 that the usual precautions with regard to charge C185001900020 collection have not been carefully observed since the C185001900021 main emphasis in this experiment was on energy C185001900022 spectra. In those cases where the continuous spectra C185001900023 are well described by the four-body shape, the C185001900024 breakup cross section is accurate to within 25 %. C185001900025 STATUS (CURVE) Fig. 5, page 125. C185001900026 ENDBIB 24 0 C185001900027 COMMON 2 3 C185001900028 EN ANG C185001900029 MEV ADEG C185001900030 7.4 105.0 C185001900031 ENDCOMMON 3 0 C185001900032 DATA 3 50 C185001900033 E-CM DATA-CM DATA-ERR C185001900034 MEV MB/SR/MEV MB/SR/MEV C185001900035 1.228 8.241E+00 C185001900036 1.299 7.845E+00 6.655E-01 C185001900037 1.362 8.323E+00 C185001900038 1.424 1.129E+01 C185001900039 1.504 1.904E+01 C185001900040 1.575 2.966E+01 C185001900041 1.655 2.687E+01 C185001900042 1.717 1.389E+01 C185001900043 1.771 6.971E+00 C185001900044 1.833 3.748E+00 C185001900045 1.966 3.785E+00 3.886E-01 C185001900046 2.028 2.603E+00 C185001900047 2.090 2.988E+00 C185001900048 2.162 2.708E+00 C185001900049 2.233 3.201E+00 C185001900050 2.304 1.844E+00 C185001900051 2.348 2.055E+00 C185001900052 2.419 1.956E+00 C185001900053 2.473 2.382E+00 C185001900054 2.588 1.544E+00 2.509E-01 C185001900055 2.713 1.485E+00 C185001900056 2.757 1.976E+00 C185001900057 2.810 8.553E-01 C185001900058 2.828 1.281E+00 C185001900059 2.935 1.083E+00 C185001900060 2.997 9.531E-01 C185001900061 3.077 1.021E+00 C185001900062 3.130 1.293E+00 C185001900063 3.193 1.052E+00 1.881E-01 C185001900064 3.299 7.983E-01 C185001900065 3.379 1.073E+00 C185001900066 3.530 1.219E+00 C185001900067 3.592 7.163E-01 C185001900068 3.655 8.553E-01 C185001900069 3.708 8.637E-01 2.273E-01 C185001900070 3.779 1.073E+00 C185001900071 3.859 1.544E+00 C185001900072 3.904 2.159E+00 C185001900073 3.975 3.233E+00 C185001900074 4.055 7.040E+00 C185001900075 4.117 1.309E+01 C185001900076 4.232 1.445E+01 1.226E+00 C185001900077 4.330 1.118E+01 C185001900078 4.384 8.743E+00 C185001900079 4.437 3.937E+00 C185001900080 4.446 2.930E+00 C185001900081 4.508 1.862E+00 C185001900082 4.526 8.984E-01 C185001900083 4.543 4.509E-01 C185001900084 4.588 4.208E-01 C185001900085 ENDDATA 52 0 C185001900086 ENDSUBENT 85 0 C185001999999 SUBENT C1850020 20180315 C174C185002000001 BIB 7 24 C185002000002 REACTION (4-BE-9(P,X)0-NN-1,,DA/DE) C185002000003 SAMPLE A 1.28 mg/cm2 Be target evaporated on a 0.5 mm thick C185002000004 tantalum plate which was thick enough to stop the C185002000005 proton beam. C185002000006 DETECTOR (SCIN) The neutron detectors, consisting of 5 x 5 cm C185002000007 plastic scintillators mounted on RCA-6655 C185002000008 photomultipliers, were positioned, at 15 degree C185002000009 angular intervals in a well collimated and shielded C185002000010 geometry. C185002000011 METHOD (TOF) The neutron spectra were observed using time-of- C185002000012 flight techniques. A flight-path of about 10 m was C185002000013 chosen as an optimum considering neutron intensities C185002000014 and resolution of the experimental equipment. C185002000015 REL-REF (M,,J.D.Anderson+,J,NIM,15,178,1962) C185002000016 ERR-ANALYS (DATA-ERR) The absolute differential cross sections C185002000017 for the ground state group are accurate to within C185002000018 about 25%. The large uncertainty is due to the fact C185002000019 that the usual precautions with regard to charge C185002000020 collection have not been carefully observed since the C185002000021 main emphasis in this experiment was on energy C185002000022 spectra. In those cases where the continuous spectra C185002000023 are well described by the four-body shape, the C185002000024 breakup cross section is accurate to within 25 %. C185002000025 STATUS (CURVE) Fig. 6, page 125. C185002000026 ENDBIB 24 0 C185002000027 COMMON 2 3 C185002000028 EN ANG C185002000029 MEV ADEG C185002000030 6.3 3.0 C185002000031 ENDCOMMON 3 0 C185002000032 DATA 3 85 C185002000033 E-CM DATA-CM DATA-ERR C185002000034 MEV MB/SR/MEV MB/SR/MEV C185002000035 0.818 1.073E+01 8.390E-01 C185002000036 0.870 1.184E+01 C185002000037 0.898 1.371E+01 C185002000038 0.941 1.317E+01 C185002000039 1.031 1.129E+01 C185002000040 1.059 1.383E+01 C185002000041 1.097 1.477E+01 C185002000042 1.101 1.538E+01 C185002000043 1.149 1.590E+01 C185002000044 1.191 2.063E+01 C185002000045 1.232 3.025E+01 C185002000046 1.303 4.400E+01 3.107E+00 C185002000047 1.346 3.448E+01 C185002000048 1.394 2.296E+01 C185002000049 1.433 1.456E+01 C185002000050 1.477 9.465E+00 C185002000051 1.558 6.203E+00 C185002000052 1.610 6.105E+00 C185002000053 1.692 3.905E+00 C185002000054 1.730 3.906E+00 C185002000055 1.768 3.486E+00 C185002000056 1.815 3.662E+00 C185002000057 1.858 2.965E+00 C185002000058 1.901 2.824E+00 C185002000059 1.949 1.836E+00 C185002000060 2.035 1.852E+00 3.772E-01 C185002000061 2.071 3.327E+00 C185002000062 2.104 3.383E+00 C185002000063 2.190 2.347E+00 C185002000064 2.214 2.027E+00 C185002000065 2.228 2.740E+00 C185002000066 2.247 2.348E+00 C185002000067 2.280 2.506E+00 C185002000068 2.289 3.122E+00 C185002000069 2.314 1.855E+00 C185002000070 2.329 1.539E+00 C185002000071 2.352 1.669E+00 C185002000072 2.366 2.350E+00 C185002000073 2.384 2.591E+00 C185002000074 2.400 1.725E+00 C185002000075 2.418 1.841E+00 C185002000076 2.419 1.419E+00 C185002000077 2.452 1.341E+00 C185002000078 2.477 1.042E+00 C185002000079 2.489 1.950E+00 C185002000080 2.524 1.237E+00 4.527E-01 C185002000081 2.594 1.984E+00 C185002000082 2.594 1.700E+00 C185002000083 2.631 2.067E+00 C185002000084 2.641 1.714E+00 C185002000085 2.672 7.062E-01 C185002000086 2.689 1.555E+00 C185002000087 2.708 1.249E+00 C185002000088 2.746 1.446E+00 C185002000089 2.756 1.209E+00 C185002000090 2.769 1.831E+00 C185002000091 2.793 1.389E+00 C185002000092 2.819 6.412E-01 C185002000093 2.837 9.173E-01 C185002000094 2.870 8.738E-01 C185002000095 2.892 1.570E+00 C185002000096 2.907 1.424E+00 C185002000097 2.936 1.324E+00 C185002000098 2.945 1.379E+00 C185002000099 2.983 1.144E+00 4.587E-01 C185002000100 3.041 7.314E-01 C185002000101 3.078 1.064E+00 C185002000102 3.113 6.169E-01 C185002000103 3.125 1.598E+00 C185002000104 3.190 2.461E+00 C185002000105 3.213 3.667E+00 C185002000106 3.258 7.385E+00 C185002000107 3.286 1.031E+01 C185002000108 3.337 1.736E+01 C185002000109 3.360 2.199E+01 C185002000110 3.379 2.405E+01 C185002000111 3.445 2.785E+01 2.998E+00 C185002000112 3.507 2.165E+01 C185002000113 3.540 1.871E+01 C185002000114 3.579 1.319E+01 C185002000115 3.594 1.033E+01 C185002000116 3.628 7.838E+00 C185002000117 3.657 4.545E+00 C185002000118 3.687 2.978E+00 C185002000119 3.712 1.386E+00 C185002000120 ENDDATA 87 0 C185002000121 ENDSUBENT 120 0 C185002099999 SUBENT C1850021 20180315 C174C185002100001 BIB 7 24 C185002100002 REACTION (4-BE-9(P,X)0-NN-1,,DA/DE) C185002100003 SAMPLE A 1.28 mg/cm2 Be target evaporated on a 0.5 mm thick C185002100004 tantalum plate which was thick enough to stop the C185002100005 proton beam. C185002100006 DETECTOR (SCIN) The neutron detectors, consisting of 5 x 5 cm C185002100007 plastic scintillators mounted on RCA-6655 C185002100008 photomultipliers, were positioned, at 15 degree C185002100009 angular intervals in a well collimated and shielded C185002100010 geometry. C185002100011 METHOD (TOF) The neutron spectra were observed using time-of- C185002100012 flight techniques. A flight-path of about 10 m was C185002100013 chosen as an optimum considering neutron intensities C185002100014 and resolution of the experimental equipment. C185002100015 REL-REF (M,,J.D.Anderson+,J,NIM,15,178,1962) C185002100016 ERR-ANALYS (DATA-ERR) The absolute differential cross sections C185002100017 for the ground state group are accurate to within C185002100018 about 25%. The large uncertainty is due to the fact C185002100019 that the usual precautions with regard to charge C185002100020 collection have not been carefully observed since the C185002100021 main emphasis in this experiment was on energy C185002100022 spectra. In those cases where the continuous spectra C185002100023 are well described by the four-body shape, the C185002100024 breakup cross section is accurate to within 25 %. C185002100025 STATUS (CURVE) Fig. 6, page 125. C185002100026 ENDBIB 24 0 C185002100027 COMMON 2 3 C185002100028 EN ANG C185002100029 MEV ADEG C185002100030 6.3 15.0 C185002100031 ENDCOMMON 3 0 C185002100032 DATA 3 96 C185002100033 E-CM DATA-CM DATA-ERR C185002100034 MEV MB/SR/MEV MB/SR/MEV C185002100035 0.832 1.270E+01 8.042E-01 C185002100036 0.885 1.230E+01 C185002100037 0.917 1.425E+01 C185002100038 0.960 1.368E+01 C185002100039 0.993 1.314E+01 C185002100040 1.041 1.438E+01 C185002100041 1.083 1.486E+01 C185002100042 1.111 1.561E+01 C185002100043 1.163 1.980E+01 C185002100044 1.200 2.884E+01 C185002100045 1.246 4.378E+01 C185002100046 1.303 4.832E+01 C185002100047 1.322 3.812E+01 C185002100048 1.371 2.554E+01 C185002100049 1.424 1.490E+01 C185002100050 1.463 1.128E+01 C185002100051 1.496 8.687E+00 7.463E-01 C185002100052 1.534 8.833E+00 C185002100053 1.625 6.531E+00 C185002100054 1.668 5.457E+00 C185002100055 1.753 5.073E+00 C185002100056 1.801 4.103E+00 C185002100057 1.844 3.844E+00 C185002100058 1.872 4.207E+00 C185002100059 1.915 3.458E+00 C185002100060 1.958 3.663E+00 C185002100061 1.991 3.755E+00 5.401E-01 C185002100062 2.053 3.695E+00 C185002100063 2.086 3.519E+00 C185002100064 2.138 3.638E+00 C185002100065 2.218 3.854E+00 C185002100066 2.223 3.409E+00 C185002100067 2.257 2.992E+00 C185002100068 2.280 3.553E+00 C185002100069 2.294 3.763E+00 C185002100070 2.318 3.612E+00 C185002100071 2.333 3.018E+00 C185002100072 2.347 3.275E+00 C185002100073 2.352 2.781E+00 C185002100074 2.389 3.044E+00 C185002100075 2.390 2.737E+00 C185002100076 2.422 3.414E+00 C185002100077 2.428 2.671E+00 C185002100078 2.456 2.783E+00 C185002100079 2.479 3.500E+00 C185002100080 2.489 2.853E+00 C185002100081 2.490 2.307E+00 C185002100082 2.508 2.673E+00 4.763E-01 C185002100083 2.537 2.652E+00 C185002100084 2.565 3.023E+00 C185002100085 2.579 2.546E+00 C185002100086 2.589 2.059E+00 C185002100087 2.622 2.927E+00 C185002100088 2.631 2.568E+00 C185002100089 2.655 2.764E+00 C185002100090 2.669 2.880E+00 C185002100091 2.684 2.387E+00 C185002100092 2.722 2.387E+00 C185002100093 2.741 2.218E+00 C185002100094 2.756 1.680E+00 C185002100095 2.760 1.868E+00 C185002100096 2.779 2.255E+00 C185002100097 2.793 2.028E+00 C185002100098 2.816 2.408E+00 C185002100099 2.840 2.275E+00 C185002100100 2.869 1.824E+00 C185002100101 2.878 1.980E+00 C185002100102 2.883 2.097E+00 C185002100103 2.944 2.511E+00 C185002100104 2.960 1.213E+00 C185002100105 2.983 1.767E+00 C185002100106 3.020 1.950E+00 C185002100107 3.049 1.812E+00 C185002100108 3.073 1.783E+00 C185002100109 3.086 2.279E+00 C185002100110 3.115 2.279E+00 C185002100111 3.143 2.598E+00 C185002100112 3.165 5.935E+00 C185002100113 3.197 7.342E+00 C185002100114 3.206 1.035E+01 C185002100115 3.229 1.448E+01 C185002100116 3.247 1.944E+01 C185002100117 3.289 2.526E+01 C185002100118 3.303 3.049E+01 C185002100119 3.374 3.681E+01 2.613E+00 C185002100120 3.412 2.953E+01 C185002100121 3.431 2.743E+01 C185002100122 3.513 1.404E+01 C185002100123 3.547 9.562E+00 C185002100124 3.563 5.179E+00 C185002100125 3.612 3.020E+00 C185002100126 3.642 1.532E+00 C185002100127 3.667 6.990E-01 C185002100128 3.687 4.315E-01 C185002100129 3.703 1.952E-01 C185002100130 3.740 2.686E-01 C185002100131 ENDDATA 98 0 C185002100132 ENDSUBENT 131 0 C185002199999 SUBENT C1850022 20180315 C174C185002200001 BIB 7 24 C185002200002 REACTION (4-BE-9(P,X)0-NN-1,,DA/DE) C185002200003 SAMPLE A 1.28 mg/cm2 Be target evaporated on a 0.5 mm thick C185002200004 tantalum plate which was thick enough to stop the C185002200005 proton beam. C185002200006 DETECTOR (SCIN) The neutron detectors, consisting of 5 x 5 cm C185002200007 plastic scintillators mounted on RCA-6655 C185002200008 photomultipliers, were positioned, at 15 degree C185002200009 angular intervals in a well collimated and shielded C185002200010 geometry. C185002200011 METHOD (TOF) The neutron spectra were observed using time-of- C185002200012 flight techniques. A flight-path of about 10 m was C185002200013 chosen as an optimum considering neutron intensities C185002200014 and resolution of the experimental equipment. C185002200015 REL-REF (M,,J.D.Anderson+,J,NIM,15,178,1962) C185002200016 ERR-ANALYS (DATA-ERR) The absolute differential cross sections C185002200017 for the ground state group are accurate to within C185002200018 about 25%. The large uncertainty is due to the fact C185002200019 that the usual precautions with regard to charge C185002200020 collection have not been carefully observed since the C185002200021 main emphasis in this experiment was on energy C185002200022 spectra. In those cases where the continuous spectra C185002200023 are well described by the four-body shape, the C185002200024 breakup cross section is accurate to within 25 %. C185002200025 STATUS (CURVE) Fig. 6, page 125. C185002200026 ENDBIB 24 0 C185002200027 COMMON 2 3 C185002200028 EN ANG C185002200029 MEV ADEG C185002200030 6.3 45.0 C185002200031 ENDCOMMON 3 0 C185002200032 DATA 3 80 C185002200033 E-CM DATA-CM DATA-ERR C185002200034 MEV MB/SR/MEV MB/SR/MEV C185002200035 1.004 9.106E+00 1.314E+00 C185002200036 1.122 1.255E+01 C185002200037 1.169 1.528E+01 C185002200038 1.201 2.304E+01 C185002200039 1.309 3.201E+01 3.237E+00 C185002200040 1.348 2.630E+01 C185002200041 1.391 1.582E+01 C185002200042 1.430 1.094E+01 C185002200043 1.473 8.625E+00 C185002200044 1.516 7.323E+00 7.404E-01 C185002200045 1.607 6.168E+00 C185002200046 1.702 6.223E+00 C185002200047 1.735 5.196E+00 C185002200048 1.792 4.376E+00 C185002200049 1.826 4.270E+00 C185002200050 1.859 4.487E+00 C185002200051 1.915 4.526E+00 C185002200052 1.953 4.640E+00 C185002200053 2.015 4.071E+00 3.815E-01 C185002200054 2.058 3.876E+00 C185002200055 2.095 4.421E+00 C185002200056 2.143 3.815E+00 C185002200057 2.181 4.042E+00 C185002200058 2.229 3.634E+00 C185002200059 2.271 4.011E+00 C185002200060 2.323 3.637E+00 C185002200061 2.366 3.138E+00 C185002200062 2.452 2.917E+00 C185002200063 2.486 2.172E+00 C185002200064 2.514 2.172E+00 5.014E-01 C185002200065 2.542 3.091E+00 C185002200066 2.561 2.085E+00 C185002200067 2.575 2.848E+00 C185002200068 2.613 2.668E+00 C185002200069 2.632 2.321E+00 C185002200070 2.655 3.068E+00 C185002200071 2.694 2.380E+00 C185002200072 2.694 1.831E+00 C185002200073 2.708 2.020E+00 C185002200074 2.732 1.715E+00 C185002200075 2.741 2.158E+00 C185002200076 2.761 1.816E+00 C185002200077 2.784 2.158E+00 C185002200078 2.794 1.893E+00 C185002200079 2.823 1.581E+00 C185002200080 2.842 1.493E+00 C185002200081 2.855 1.909E+00 C185002200082 2.878 2.422E+00 C185002200083 2.898 1.990E+00 C185002200084 2.927 1.760E+00 C185002200085 2.945 1.789E+00 C185002200086 2.968 2.384E+00 C185002200087 2.997 2.179E+00 3.747E-01 C185002200088 3.026 1.880E+00 C185002200089 3.044 2.253E+00 C185002200090 3.087 1.960E+00 C185002200091 3.096 2.406E+00 C185002200092 3.101 2.634E+00 C185002200093 3.115 2.426E+00 C185002200094 3.129 3.129E+00 C185002200095 3.152 4.874E+00 C185002200096 3.179 6.390E+00 C185002200097 3.217 7.229E+00 C185002200098 3.249 1.273E+01 C185002200099 3.272 1.739E+01 C185002200100 3.290 2.050E+01 C185002200101 3.351 3.355E+01 C185002200102 3.370 3.672E+01 C185002200103 3.393 3.383E+01 C185002200104 3.412 3.584E+01 3.624E+00 C185002200105 3.460 3.276E+01 C185002200106 3.465 2.826E+01 C185002200107 3.494 2.459E+01 C185002200108 3.523 1.923E+01 C185002200109 3.538 1.351E+01 C185002200110 3.596 5.904E+00 C185002200111 3.641 2.687E+00 C185002200112 3.647 1.656E+00 C185002200113 3.681 1.136E+00 C185002200114 3.723 1.155E+00 C185002200115 ENDDATA 82 0 C185002200116 ENDSUBENT 115 0 C185002299999 SUBENT C1850023 20180315 C174C185002300001 BIB 7 24 C185002300002 REACTION (3-LI-6(A,X)0-NN-1,,DA/DE) C185002300003 SAMPLE (3-LI-6,ENR=0.93) a 1.3 mg/cm2 Li6 target (93% C185002300004 enriched) evaporated on a gold backing about 0.25 mm C185002300005 thick. C185002300006 DETECTOR (SCIN) The neutron detectors, consisting of 5 x 5 cm C185002300007 plastic scintillators mounted on RCA-6655 C185002300008 photomultipliers, were positioned, at 15 degree C185002300009 angular intervals in a well collimated and shielded C185002300010 geometry. C185002300011 METHOD (TOF) The neutron spectra were observed using time-of- C185002300012 flight techniques. A flight-path of about 10 m was C185002300013 chosen as an optimum considering neutron intensities C185002300014 and resolution of the experimental equipment. C185002300015 REL-REF (M,,J.D.Anderson+,J,NIM,15,178,1962) C185002300016 ERR-ANALYS (DATA-ERR) The absolute differential cross sections C185002300017 for the ground state group are accurate to within C185002300018 about 25%. The large uncertainty is due to the fact C185002300019 that the usual precautions with regard to charge C185002300020 collection have not been carefully observed since the C185002300021 main emphasis in this experiment was on energy C185002300022 spectra. In those cases where the continuous spectra C185002300023 are well described by the four-body shape, the C185002300024 breakup cross section is accurate to within 25 %. C185002300025 STATUS (CURVE) Fig. 7, page 126. C185002300026 ENDBIB 24 0 C185002300027 COMMON 2 3 C185002300028 EN ANG C185002300029 MEV ADEG C185002300030 14.4 15.0 C185002300031 ENDCOMMON 3 0 C185002300032 DATA 3 122 C185002300033 E-CM DATA-CM DATA-ERR C185002300034 MEV MB/SR/MEV MB/SR/MEV C185002300035 0.166 2.344E+00 C185002300036 0.181 2.775E+00 C185002300037 0.217 3.369E+00 C185002300038 0.260 4.302E+00 C185002300039 0.304 4.450E+00 C185002300040 0.304 3.988E+00 C185002300041 0.325 4.160E+00 C185002300042 0.354 4.056E+00 C185002300043 0.383 4.302E+00 C185002300044 0.412 4.056E+00 C185002300045 0.427 4.526E+00 C185002300046 0.484 3.954E+00 C185002300047 0.520 4.883E+00 C185002300048 0.535 3.514E+00 C185002300049 0.542 4.160E+00 C185002300050 0.542 3.855E+00 C185002300051 0.564 3.285E+00 C185002300052 0.586 4.966E+00 C185002300053 0.586 3.791E+00 C185002300054 0.614 4.090E+00 C185002300055 0.622 4.266E+00 C185002300056 0.629 3.397E+00 C185002300057 0.629 3.759E+00 C185002300058 0.636 3.257E+00 C185002300059 0.658 3.484E+00 C185002300060 0.665 2.968E+00 C185002300061 0.665 3.988E+00 C185002300062 0.672 2.798E+00 C185002300063 0.687 3.791E+00 C185002300064 0.694 2.616E+00 C185002300065 0.708 3.696E+00 C185002300066 0.730 3.514E+00 C185002300067 0.737 3.791E+00 C185002300068 0.737 4.266E+00 C185002300069 0.773 3.514E+00 C185002300070 0.781 4.266E+00 C185002300071 0.795 3.312E+00 C185002300072 0.817 3.514E+00 C185002300073 0.817 3.921E+00 C185002300074 0.824 3.759E+00 C185002300075 0.846 4.125E+00 C185002300076 0.846 4.450E+00 C185002300077 0.882 3.988E+00 C185002300078 0.889 4.642E+00 C185002300079 0.896 3.123E+00 C185002300080 0.925 4.339E+00 C185002300081 0.947 5.008E+00 C185002300082 0.983 4.564E+00 C185002300083 1.005 4.230E+00 C185002300084 1.019 4.375E+00 C185002300085 1.041 4.883E+00 5.438E-01 C185002300086 1.077 4.302E+00 C185002300087 1.106 4.266E+00 C185002300088 1.113 3.634E+00 C185002300089 1.128 3.921E+00 C185002300090 1.157 4.603E+00 C185002300091 1.178 3.312E+00 C185002300092 1.200 4.160E+00 C185002300093 1.200 3.888E+00 C185002300094 1.229 4.603E+00 C185002300095 1.287 4.842E+00 C185002300096 1.301 3.988E+00 C185002300097 1.316 4.603E+00 C185002300098 1.316 3.823E+00 C185002300099 1.345 3.514E+00 C185002300100 1.366 3.791E+00 C185002300101 1.388 3.954E+00 C185002300102 1.388 3.604E+00 C185002300103 1.424 3.791E+00 C185002300104 1.453 3.544E+00 C185002300105 1.475 3.176E+00 C185002300106 1.489 3.888E+00 C185002300107 1.525 3.285E+00 C185002300108 1.547 2.728E+00 1.994E-01 C185002300109 1.576 2.919E+00 C185002300110 1.605 2.572E+00 C185002300111 1.612 2.728E+00 C185002300112 1.634 2.305E+00 C185002300113 1.648 2.508E+00 C185002300114 1.684 2.344E+00 C185002300115 1.720 2.228E+00 C185002300116 1.771 2.364E+00 C185002300117 1.807 2.822E+00 C185002300118 1.843 1.964E+00 C185002300119 1.858 2.154E+00 C185002300120 1.880 1.805E+00 C185002300121 1.894 2.065E+00 C185002300122 1.923 2.247E+00 C185002300123 1.952 2.048E+00 C185002300124 1.988 2.247E+00 C185002300125 2.039 1.980E+00 C185002300126 2.096 1.659E+00 C185002300127 2.176 1.026E+00 C185002300128 2.292 8.167E-01 C185002300129 2.443 4.450E-01 C185002300130 2.559 3.921E-01 4.367E-02 C185002300131 2.704 3.604E-01 C185002300132 2.812 3.096E-01 C185002300133 2.949 3.257E-01 C185002300134 2.993 2.572E-01 C185002300135 3.065 2.508E-01 3.532E-02 C185002300136 3.202 2.487E-01 C185002300137 3.318 3.019E-01 C185002300138 3.361 3.855E-01 C185002300139 3.427 4.681E-01 C185002300140 3.484 3.397E-01 6.919E-02 C185002300141 3.528 5.136E-01 C185002300142 3.607 5.312E-01 C185002300143 3.665 6.958E-01 C185002300144 3.701 8.962E-01 C185002300145 3.752 1.061E+00 C185002300146 3.817 1.043E+00 C185002300147 3.867 1.288E+00 C185002300148 4.005 1.245E+00 1.007E-01 C185002300149 4.048 1.310E+00 C185002300150 4.135 1.194E+00 C185002300151 4.193 8.886E-01 C185002300152 4.323 7.963E-01 C185002300153 4.431 4.842E-01 C185002300154 4.561 2.798E-01 C185002300155 4.742 2.173E-01 C185002300156 4.829 1.898E-01 C185002300157 ENDDATA 124 0 C185002300158 ENDSUBENT 157 0 C185002399999 SUBENT C1850024 20180315 C174C185002400001 BIB 7 24 C185002400002 REACTION (3-LI-6(A,X)0-NN-1,,DA/DE) C185002400003 SAMPLE (3-LI-6,ENR=0.93) a 1.3 mg/cm2 Li6 target (93% C185002400004 enriched) evaporated on a gold backing about 0.25 mm C185002400005 thick. C185002400006 DETECTOR (SCIN) The neutron detectors, consisting of 5 x 5 cm C185002400007 plastic scintillators mounted on RCA-6655 C185002400008 photomultipliers, were positioned, at 15 degree C185002400009 angular intervals in a well collimated and shielded C185002400010 geometry. C185002400011 METHOD (TOF) The neutron spectra were observed using time-of- C185002400012 flight techniques. A flight-path of about 10 m was C185002400013 chosen as an optimum considering neutron intensities C185002400014 and resolution of the experimental equipment. C185002400015 REL-REF (M,,J.D.Anderson+,J,NIM,15,178,1962) C185002400016 ERR-ANALYS (DATA-ERR) The absolute differential cross sections C185002400017 for the ground state group are accurate to within C185002400018 about 25%. The large uncertainty is due to the fact C185002400019 that the usual precautions with regard to charge C185002400020 collection have not been carefully observed since the C185002400021 main emphasis in this experiment was on energy C185002400022 spectra. In those cases where the continuous spectra C185002400023 are well described by the four-body shape, the C185002400024 breakup cross section is accurate to within 25 %. C185002400025 STATUS (CURVE) Fig. 7, page 126. C185002400026 ENDBIB 24 0 C185002400027 COMMON 2 3 C185002400028 EN ANG C185002400029 MEV ADEG C185002400030 14.4 30.0 C185002400031 ENDCOMMON 3 0 C185002400032 DATA 3 120 C185002400033 E-CM DATA-CM DATA-ERR C185002400034 MEV MB/SR/MEV MB/SR/MEV C185002400035 0.239 1.077E+00 C185002400036 0.267 1.281E+00 C185002400037 0.289 1.872E+00 C185002400038 0.311 2.208E+00 C185002400039 0.369 2.320E+00 C185002400040 0.369 2.737E+00 C185002400041 0.398 3.149E+00 C185002400042 0.419 3.448E+00 C185002400043 0.434 3.047E+00 C185002400044 0.463 3.255E+00 C185002400045 0.484 3.477E+00 C185002400046 0.506 3.282E+00 C185002400047 0.549 2.924E+00 C185002400048 0.607 3.072E+00 C185002400049 0.614 3.336E+00 C185002400050 0.643 2.829E+00 C185002400051 0.651 2.972E+00 C185002400052 0.716 2.997E+00 C185002400053 0.752 2.245E+00 C185002400054 0.766 2.829E+00 C185002400055 0.773 2.948E+00 C185002400056 0.788 2.499E+00 C185002400057 0.810 3.364E+00 C185002400058 0.817 2.398E+00 C185002400059 0.824 2.852E+00 C185002400060 0.831 2.190E+00 C185002400061 0.846 2.541E+00 C185002400062 0.875 2.924E+00 C185002400063 0.875 3.255E+00 C185002400064 0.882 2.340E+00 C185002400065 0.896 3.506E+00 C185002400066 0.904 2.208E+00 C185002400067 0.940 2.714E+00 C185002400068 0.947 2.900E+00 C185002400069 0.961 3.255E+00 C185002400070 1.027 2.972E+00 2.355E-01 C185002400071 1.041 2.499E+00 C185002400072 1.063 2.714E+00 C185002400073 1.070 3.282E+00 C185002400074 1.077 3.839E+00 C185002400075 1.084 2.852E+00 C185002400076 1.106 3.047E+00 C185002400077 1.128 3.684E+00 C185002400078 1.135 2.997E+00 C185002400079 1.149 2.805E+00 C185002400080 1.157 3.282E+00 C185002400081 1.186 2.997E+00 C185002400082 1.193 2.438E+00 C185002400083 1.229 3.282E+00 C185002400084 1.236 2.137E+00 C185002400085 1.243 2.782E+00 C185002400086 1.251 2.418E+00 C185002400087 1.272 2.626E+00 C185002400088 1.294 2.997E+00 C185002400089 1.323 2.876E+00 C185002400090 1.330 2.670E+00 C185002400091 1.337 3.072E+00 C185002400092 1.359 3.448E+00 C185002400093 1.366 2.876E+00 C185002400094 1.373 2.398E+00 C185002400095 1.388 2.737E+00 C185002400096 1.402 3.022E+00 C185002400097 1.410 2.418E+00 C185002400098 1.431 3.149E+00 C185002400099 1.453 2.479E+00 1.775E-01 C185002400100 1.489 2.900E+00 C185002400101 1.518 2.379E+00 C185002400102 1.540 2.520E+00 C185002400103 1.547 2.438E+00 C185002400104 1.569 2.301E+00 C185002400105 1.590 2.208E+00 C185002400106 1.605 2.067E+00 C185002400107 1.627 2.924E+00 C185002400108 1.655 2.208E+00 C185002400109 1.684 1.668E+00 C185002400110 1.713 2.000E+00 C185002400111 1.735 1.724E+00 C185002400112 1.749 1.346E+00 C185002400113 1.757 1.498E+00 C185002400114 1.793 1.474E+00 C185002400115 1.829 1.710E+00 C185002400116 1.865 1.281E+00 C185002400117 1.923 1.919E+00 C185002400118 1.945 1.523E+00 C185002400119 1.988 2.245E+00 C185002400120 1.995 2.670E+00 1.706E-01 C185002400121 2.060 2.759E+00 1.975E-01 C185002400122 2.067 1.826E+00 C185002400123 2.082 1.654E+00 C185002400124 2.118 2.102E+00 C185002400125 2.161 2.282E+00 C185002400126 2.190 1.826E+00 C185002400127 2.270 1.357E+00 C185002400128 2.465 5.657E-01 C185002400129 2.465 6.456E-01 C185002400130 2.588 5.209E-01 7.191E-02 C185002400131 2.718 2.084E-01 C185002400132 2.841 1.724E-01 C185002400133 2.971 2.418E-01 C185002400134 3.094 1.935E-01 3.477E-02 C185002400135 3.217 2.101E-01 C185002400136 3.361 1.983E-01 C185002400137 3.463 1.811E-01 C185002400138 3.643 2.562E-01 5.453E-02 C185002400139 3.672 4.641E-01 C185002400140 3.737 2.972E-01 C185002400141 3.846 6.403E-01 C185002400142 3.925 1.438E+00 C185002400143 4.005 1.511E+00 C185002400144 4.041 1.842E+00 C185002400145 4.084 2.340E+00 C185002400146 4.157 2.208E+00 C185002400147 4.229 2.359E+00 1.689E-01 C185002400148 4.287 2.154E+00 C185002400149 4.352 2.137E+00 C185002400150 4.402 1.682E+00 C185002400151 4.482 1.068E+00 C185002400152 4.598 4.836E-01 C185002400153 4.670 2.828E-01 C185002400154 4.749 1.150E-01 C185002400155 ENDDATA 122 0 C185002400156 ENDSUBENT 155 0 C185002499999 SUBENT C1850025 20180315 C174C185002500001 BIB 7 24 C185002500002 REACTION (3-LI-6(A,X)0-NN-1,,DA/DE) C185002500003 SAMPLE (3-LI-6,ENR=0.93) a 1.3 mg/cm2 Li6 target (93% C185002500004 enriched) evaporated on a gold backing about 0.25 mm C185002500005 thick. C185002500006 DETECTOR (SCIN) The neutron detectors, consisting of 5 x 5 cm C185002500007 plastic scintillators mounted on RCA-6655 C185002500008 photomultipliers, were positioned, at 15 degree C185002500009 angular intervals in a well collimated and shielded C185002500010 geometry. C185002500011 METHOD (TOF) The neutron spectra were observed using time-of- C185002500012 flight techniques. A flight-path of about 10 m was C185002500013 chosen as an optimum considering neutron intensities C185002500014 and resolution of the experimental equipment. C185002500015 REL-REF (M,,J.D.Anderson+,J,NIM,15,178,1962) C185002500016 ERR-ANALYS (DATA-ERR) The absolute differential cross sections C185002500017 for the ground state group are accurate to within C185002500018 about 25%. The large uncertainty is due to the fact C185002500019 that the usual precautions with regard to charge C185002500020 collection have not been carefully observed since the C185002500021 main emphasis in this experiment was on energy C185002500022 spectra. In those cases where the continuous spectra C185002500023 are well described by the four-body shape, the C185002500024 breakup cross section is accurate to within 25 %. C185002500025 STATUS (CURVE) Fig. 7, page 126. C185002500026 ENDBIB 24 0 C185002500027 COMMON 2 3 C185002500028 EN ANG C185002500029 MEV ADEG C185002500030 14.4 45.0 C185002500031 ENDCOMMON 3 0 C185002500032 DATA 3 98 C185002500033 E-CM DATA-CM DATA-ERR C185002500034 MEV MB/SR/MEV MB/SR/MEV C185002500035 0.911 2.456E+00 C185002500036 0.947 2.542E+00 C185002500037 0.998 2.586E+00 2.531E-01 C185002500038 1.084 2.141E+00 C185002500039 1.084 2.498E+00 C185002500040 1.092 3.176E+00 C185002500041 1.092 1.759E+00 C185002500042 1.113 2.675E+00 C185002500043 1.120 2.939E+00 C185002500044 1.135 2.052E+00 C185002500045 1.157 3.230E+00 C185002500046 1.171 2.498E+00 C185002500047 1.214 2.698E+00 C185002500048 1.222 3.967E+00 C185002500049 1.229 2.520E+00 C185002500050 1.236 3.203E+00 C185002500051 1.258 3.460E+00 C185002500052 1.272 2.914E+00 C185002500053 1.287 2.653E+00 C185002500054 1.308 3.176E+00 C185002500055 1.308 3.042E+00 C185002500056 1.330 2.865E+00 C185002500057 1.345 3.095E+00 C185002500058 1.345 2.414E+00 C185002500059 1.359 2.254E+00 C185002500060 1.366 2.675E+00 C185002500061 1.395 2.456E+00 C185002500062 1.402 2.698E+00 C185002500063 1.410 3.611E+00 C185002500064 1.417 2.160E+00 C185002500065 1.431 2.890E+00 C185002500066 1.439 2.520E+00 C185002500067 1.475 2.216E+00 C185002500068 1.482 2.105E+00 C185002500069 1.496 3.286E+00 C185002500070 1.511 2.564E+00 C185002500071 1.540 2.236E+00 2.361E-01 C185002500072 1.583 2.236E+00 C185002500073 1.612 1.670E+00 C185002500074 1.641 2.160E+00 C185002500075 1.648 1.852E+00 C185002500076 1.677 2.314E+00 C185002500077 1.699 1.685E+00 C185002500078 1.728 1.949E+00 C185002500079 1.728 2.105E+00 C185002500080 1.771 2.456E+00 C185002500081 1.793 1.949E+00 C185002500082 1.829 2.564E+00 C185002500083 1.843 2.141E+00 C185002500084 1.851 3.314E+00 C185002500085 1.858 2.939E+00 C185002500086 1.901 3.121E+00 2.070E-01 C185002500087 1.908 3.900E+00 C185002500088 1.930 2.722E+00 C185002500089 1.966 3.068E+00 C185002500090 1.981 2.675E+00 C185002500091 2.046 3.176E+00 3.597E-01 C185002500092 2.089 2.675E+00 C185002500093 2.104 2.456E+00 C185002500094 2.154 1.744E+00 C185002500095 2.169 1.432E+00 C185002500096 2.219 1.729E+00 C185002500097 2.255 1.534E+00 C185002500098 2.292 7.667E-01 C185002500099 2.451 5.040E-01 C185002500100 2.566 5.633E-01 5.514E-02 C185002500101 2.704 4.433E-01 C185002500102 2.812 4.747E-01 C185002500103 3.072 3.016E-01 2.717E-02 C185002500104 3.217 2.235E-01 C185002500105 3.318 2.816E-01 C185002500106 3.448 3.174E-01 C185002500107 3.535 2.865E-01 2.128E-02 C185002500108 3.564 3.735E-01 C185002500109 3.564 3.548E-01 C185002500110 3.672 7.409E-01 C185002500111 3.745 7.098E-01 C185002500112 3.773 8.792E-01 C185002500113 3.839 8.868E-01 C185002500114 3.860 1.008E+00 C185002500115 3.904 1.715E+00 C185002500116 3.954 1.657E+00 C185002500117 3.990 2.052E+00 C185002500118 4.027 2.353E+00 C185002500119 4.106 2.414E+00 C185002500120 4.142 2.236E+00 C185002500121 4.193 2.478E+00 2.232E-01 C185002500122 4.316 2.070E+00 C185002500123 4.395 2.070E+00 C185002500124 4.439 1.670E+00 C185002500125 4.511 1.600E+00 C185002500126 4.576 1.166E+00 C185002500127 4.619 9.099E-01 C185002500128 4.670 5.040E-01 C185002500129 4.757 4.587E-01 C185002500130 4.814 2.607E-01 C185002500131 4.887 2.414E-01 C185002500132 4.930 1.520E-01 C185002500133 ENDDATA 100 0 C185002500134 ENDSUBENT 133 0 C185002599999 SUBENT C1850026 20180315 C174C185002600001 BIB 7 24 C185002600002 REACTION (3-LI-6(A,X)0-NN-1,,DA/DE) C185002600003 SAMPLE (3-LI-6,ENR=0.93) a 1.3 mg/cm2 Li6 target (93% C185002600004 enriched) evaporated on a gold backing about 0.25 mm C185002600005 thick. C185002600006 DETECTOR (SCIN) The neutron detectors, consisting of 5 x 5 cm C185002600007 plastic scintillators mounted on RCA-6655 C185002600008 photomultipliers, were positioned, at 15 degree C185002600009 angular intervals in a well collimated and shielded C185002600010 geometry. C185002600011 METHOD (TOF) The neutron spectra were observed using time-of- C185002600012 flight techniques. A flight-path of about 10 m was C185002600013 chosen as an optimum considering neutron intensities C185002600014 and resolution of the experimental equipment. C185002600015 REL-REF (M,,J.D.Anderson+,J,NIM,15,178,1962) C185002600016 ERR-ANALYS (DATA-ERR) The absolute differential cross sections C185002600017 for the ground state group are accurate to within C185002600018 about 25%. The large uncertainty is due to the fact C185002600019 that the usual precautions with regard to charge C185002600020 collection have not been carefully observed since the C185002600021 main emphasis in this experiment was on energy C185002600022 spectra. In those cases where the continuous spectra C185002600023 are well described by the four-body shape, the C185002600024 breakup cross section is accurate to within 25 %. C185002600025 STATUS (CURVE) Fig. 7, page 126. C185002600026 ENDBIB 24 0 C185002600027 COMMON 2 3 C185002600028 EN ANG C185002600029 MEV ADEG C185002600030 14.4 60.0 C185002600031 ENDCOMMON 3 0 C185002600032 DATA 3 82 C185002600033 E-CM DATA-CM DATA-ERR C185002600034 MEV MB/SR/MEV MB/SR/MEV C185002600035 0.983 2.708E+00 C185002600036 0.998 3.428E+00 C185002600037 1.034 3.047E+00 2.223E-01 C185002600038 1.055 2.708E+00 C185002600039 1.113 2.469E+00 C185002600040 1.193 2.731E+00 C185002600041 1.207 2.825E+00 C185002600042 1.251 3.073E+00 C185002600043 1.294 2.469E+00 C185002600044 1.337 2.731E+00 C185002600045 1.373 3.073E+00 C185002600046 1.424 3.099E+00 C185002600047 1.453 2.996E+00 C185002600048 1.511 2.139E+00 C185002600049 1.518 2.825E+00 2.061E-01 C185002600050 1.561 2.618E+00 C185002600051 1.576 2.777E+00 C185002600052 1.576 2.176E+00 C185002600053 1.590 3.151E+00 C185002600054 1.612 2.596E+00 C185002600055 1.619 1.901E+00 C185002600056 1.619 2.194E+00 C185002600057 1.648 2.448E+00 C185002600058 1.655 2.250E+00 C185002600059 1.670 2.663E+00 C185002600060 1.684 2.801E+00 C185002600061 1.684 2.194E+00 C185002600062 1.706 1.983E+00 C185002600063 1.706 1.607E+00 C185002600064 1.720 2.308E+00 C185002600065 1.720 1.763E+00 C185002600066 1.778 1.748E+00 C185002600067 1.778 2.139E+00 C185002600068 1.786 2.250E+00 C185002600069 1.814 2.176E+00 C185002600070 1.814 2.708E+00 C185002600071 1.822 2.897E+00 C185002600072 1.836 1.934E+00 C185002600073 1.843 1.748E+00 C185002600074 1.872 2.121E+00 C185002600075 1.880 2.825E+00 C185002600076 1.894 3.486E+00 C185002600077 1.908 2.596E+00 C185002600078 1.945 2.250E+00 C185002600079 1.945 5.179E+00 C185002600080 1.995 5.356E+00 C185002600081 2.060 4.091E+00 3.303E-01 C185002600082 2.096 4.376E+00 C185002600083 2.111 3.343E+00 C185002600084 2.161 4.196E+00 C185002600085 2.169 3.729E+00 C185002600086 2.219 3.343E+00 C185002600087 2.234 2.469E+00 C185002600088 2.357 1.477E+00 C185002600089 2.451 7.531E-01 C185002600090 2.559 6.102E-01 3.975E-02 C185002600091 2.696 6.694E-01 C185002600092 2.827 5.469E-01 C185002600093 2.957 6.206E-01 C185002600094 3.080 5.850E-01 5.622E-02 C185002600095 3.202 4.039E-01 C185002600096 3.325 4.394E-01 C185002600097 3.448 3.059E-01 C185002600098 3.578 5.070E-01 1.065E-01 C185002600099 3.651 5.378E-01 C185002600100 3.665 7.282E-01 C185002600101 3.716 5.704E-01 C185002600102 3.802 6.865E-01 C185002600103 3.853 7.659E-01 C185002600104 3.925 1.259E+00 C185002600105 3.961 2.176E+00 C185002600106 4.157 3.371E+00 C185002600107 4.193 2.825E+00 3.972E-01 C185002600108 4.301 2.754E+00 C185002600109 4.381 2.946E+00 C185002600110 4.395 2.000E+00 C185002600111 4.467 1.515E+00 C185002600112 4.511 1.177E+00 C185002600113 4.554 8.764E-01 C185002600114 4.590 5.469E-01 C185002600115 4.641 3.776E-01 C185002600116 4.699 1.123E-01 C185002600117 ENDDATA 84 0 C185002600118 ENDSUBENT 117 0 C185002699999 SUBENT C1850027 20180317 C174C185002700001 BIB 7 24 C185002700002 REACTION (3-LI-6(A,X)0-NN-1,,DA/DE) C185002700003 SAMPLE (3-LI-6,ENR=0.93) a 1.3 mg/cm2 Li6 target (93% C185002700004 enriched) evaporated on a gold backing about 0.25 mm C185002700005 thick. C185002700006 DETECTOR (SCIN) The neutron detectors, consisting of 5 x 5 cm C185002700007 plastic scintillators mounted on RCA-6655 C185002700008 photomultipliers, were positioned, at 15 degree C185002700009 angular intervals in a well collimated and shielded C185002700010 geometry. C185002700011 METHOD (TOF) The neutron spectra were observed using time-of- C185002700012 flight techniques. A flight-path of about 10 m was C185002700013 chosen as an optimum considering neutron intensities C185002700014 and resolution of the experimental equipment. C185002700015 REL-REF (M,,J.D.Anderson+,J,NIM,15,178,1962) C185002700016 ERR-ANALYS (DATA-ERR) The absolute differential cross sections C185002700017 for the ground state group are accurate to within C185002700018 about 25%. The large uncertainty is due to the fact C185002700019 that the usual precautions with regard to charge C185002700020 collection have not been carefully observed since the C185002700021 main emphasis in this experiment was on energy C185002700022 spectra. In those cases where the continuous spectra C185002700023 are well described by the four-body shape, the C185002700024 breakup cross section is accurate to within 25 %. C185002700025 STATUS (CURVE) Fig. 7, page 126. C185002700026 ENDBIB 24 0 C185002700027 COMMON 2 3 C185002700028 EN ANG C185002700029 MEV ADEG C185002700030 14.4 75.0 C185002700031 ENDCOMMON 3 0 C185002700032 DATA 3 44 C185002700033 E-CM DATA-CM DATA-ERR C185002700034 MEV MB/SR/MEV MB/SR/MEV C185002700035 1.569 1.951E+00 1.985E-01 C185002700036 1.648 2.033E+00 C185002700037 1.663 1.486E+00 C185002700038 1.728 1.498E+00 C185002700039 1.764 1.696E+00 C185002700040 1.800 1.335E+00 C185002700041 1.836 1.426E+00 C185002700042 1.880 1.486E+00 C185002700043 1.901 1.935E+00 C185002700044 1.952 2.137E+00 C185002700045 2.002 2.227E+00 2.100E-01 C185002700046 2.060 2.924E+00 C185002700047 2.140 2.479E+00 C185002700048 2.205 2.459E+00 C185002700049 2.227 1.767E+00 C185002700050 2.306 8.340E-01 C185002700051 2.465 5.995E-01 C185002700052 2.559 3.935E-01 9.873E-02 C185002700053 2.704 5.946E-01 C185002700054 2.834 2.033E-01 C185002700055 2.942 4.169E-01 C185002700056 3.080 2.379E-01 8.428E-02 C185002700057 3.210 2.948E-01 C185002700058 3.318 1.588E-01 C185002700059 3.441 3.364E-01 C185002700060 3.571 2.499E-01 8.036E-02 C185002700061 3.701 1.696E-01 C185002700062 3.810 1.812E-01 C185002700063 3.860 2.245E-01 C185002700064 3.875 2.852E-01 C185002700065 3.933 2.948E-01 C185002700066 3.954 1.160E+00 C185002700067 4.019 1.077E+00 C185002700068 4.041 1.812E+00 C185002700069 4.070 1.654E+00 C185002700070 4.106 2.190E+00 C185002700071 4.128 2.283E+00 C185002700072 4.178 2.102E+00 C185002700073 4.193 2.340E+00 2.380E-01 C185002700074 4.316 1.160E+00 C185002700075 4.359 6.955E-01 C185002700076 4.388 4.797E-01 C185002700077 4.431 3.123E-01 C185002700078 4.547 1.682E-01 C185002700079 ENDDATA 46 0 C185002700080 ENDSUBENT 79 0 C185002799999 SUBENT C1850028 20180315 C174C185002800001 BIB 4 8 C185002800002 REACTION (6-C-12(P,A)5-B-9,PAR,DA) C185002800003 ANALYSIS Authors say that the cs is "roughly constant" in this C185002800004 energy range 14.3 - 18.3 MeV. C185002800005 ERR-ANALYS (DATA-ERR) No details given C185002800006 STATUS (DEP,C1850003) C185002800007 (DEP,C1850004) C185002800008 (DEP,C1850005) C185002800009 (TABLE) page 123. C185002800010 ENDBIB 8 0 C185002800011 COMMON 5 3 C185002800012 EN-MIN EN-MAX ANG-MIN ANG-MAX E-LVL C185002800013 MEV MEV ADEG ADEG MEV C185002800014 14.3 18.3 86.0 90.0 0.0 C185002800015 ENDCOMMON 3 0 C185002800016 DATA 2 1 C185002800017 DATA DATA-ERR C185002800018 MB/SR MB/SR C185002800019 2.0 0.5 C185002800020 ENDDATA 3 0 C185002800021 ENDSUBENT 20 0 C185002899999 SUBENT C1850029 20180315 C174C185002900001 BIB 3 10 C185002900002 REACTION (4-BE-9(P,N)5-B-9,PAR,DA) C185002900003 EN-SEC (E-LVL,4-BE-9) C185002900004 STATUS (DEP,C1850016) C185002900005 (DEP,C1850017) C185002900006 (DEP,C1850018) C185002900007 (DEP,C1850019) C185002900008 (DEP,C1850020) C185002900009 (DEP,C1850021) C185002900010 (DEP,C1850022) C185002900011 (TABLE) page 126. C185002900012 ENDBIB 10 0 C185002900013 COMMON 5 3 C185002900014 EN-MIN EN-MAX ANG-MIN ANG-MAX E-LVL C185002900015 MEV MEV ADEG ADEG MEV C185002900016 6.3 7.4 3.0 105.0 1.7 C185002900017 ENDCOMMON 3 0 C185002900018 DATA 1 1 C185002900019 DATA-MAX C185002900020 MB/SR C185002900021 0.1 C185002900022 ENDDATA 3 0 C185002900023 ENDSUBENT 22 0 C185002999999 SUBENT C1850030 20180315 C174C185003000001 BIB 3 7 C185003000002 REACTION (3-LI-6(A,N)5-B-9,PAR,DA) C185003000003 ERR-ANALYS (DATA-ERR) No details given C185003000004 STATUS (DEP,C1850023) C185003000005 (DEP,C1850024) C185003000006 (DEP,C1850025) C185003000007 (DEP,C1850026) C185003000008 (TABLE) page 126. C185003000009 ENDBIB 7 0 C185003000010 COMMON 4 3 C185003000011 EN ANG-MIN ANG-MAX E-LVL C185003000012 MEV ADEG ADEG MEV C185003000013 14.4 15.0 60.0 0.0 C185003000014 ENDCOMMON 3 0 C185003000015 DATA 2 1 C185003000016 DATA DATA-ERR C185003000017 MB/SR MB/SR C185003000018 1.0 0.25 C185003000019 ENDDATA 3 0 C185003000020 ENDSUBENT 19 0 C185003099999 SUBENT C1850031 20180315 C174C185003100001 BIB 2 3 C185003100002 REACTION (3-LI-6(A,N)5-B-9,PAR,DA) C185003100003 STATUS (DEP,C1850027) C185003100004 (TABLE) page 126. C185003100005 ENDBIB 3 0 C185003100006 COMMON 3 3 C185003100007 EN ANG E-LVL C185003100008 MEV ADEG MEV C185003100009 14.4 75.0 0.0 C185003100010 ENDCOMMON 3 0 C185003100011 DATA 1 1 C185003100012 DATA C185003100013 MB/SR C185003100014 0.6 C185003100015 ENDDATA 3 0 C185003100016 ENDSUBENT 15 0 C185003199999 ENDENTRY 31 0 C185099999999