ENTRY C1850 20180315 C174C1850 0 1 SUBENT C1850001 20180315 C174C1850 1 1 BIB 6 8 C1850 1 2 TITLE A search for an excited state of B9 near 1.7 MeV C1850 1 3 AUTHOR (R.W.Bauer,J.D.Anderson,C.Wong) C1850 1 4 REFERENCE (J,NP,56,117,1964) C1850 1 5 #doi:10.1016/0029-5582(64)90458-4 C1850 1 6 INSTITUTE (1USALRL) C1850 1 7 FACILITY (CYCLO,1USALRL) Livermore 230 cm variable energy C1850 1 8 cyclotron. C1850 1 9 HISTORY (20180315C) BP C1850 1 10 ENDBIB 8 0 C1850 1 11 NOCOMMON 0 0 C1850 1 12 ENDSUBENT 11 0 C1850 199999 SUBENT C1850002 20180315 C174C1850 2 1 BIB 5 18 C1850 2 2 REACTION (6-C-12(P,X)2-HE-4,,DA/DE) C1850 2 3 SAMPLE A thin self-supported polystyrene (CH) target located C1850 2 4 at the center of a 1 m diam. scattering chamber. C1850 2 5 Targets of thicknesses ranging from 50 to C1850 2 6 150 microg/cm2 were used. C1850 2 7 DETECTOR (SIBAR) The alpha spectra were measured using a thin C1850 2 8 Ortec Surface Barrier detector (50 microm thickness, C1850 2 9 totally depleted at a reverse bias of about 100 V). C1850 2 10 ERR-ANALYS (DATA-ERR) The absolute differential cross sections C1850 2 11 for the ground state group are accurate to within C1850 2 12 about 25%. The large uncertainty is due to the fact C1850 2 13 that the usual precautions with regard to charge C1850 2 14 collection have not been carefully observed since the C1850 2 15 main emphasis in this experiment was on energy C1850 2 16 spectra. In those cases where the continuous spectra C1850 2 17 are well described by the four-body shape, the C1850 2 18 breakup cross section is accurate to within 25 %. C1850 2 19 STATUS (CURVE) Fig. 1, page 121. C1850 2 20 ENDBIB 18 0 C1850 2 21 COMMON 2 3 C1850 2 22 EN ANG C1850 2 23 MEV ADEG C1850 2 24 12.7 45.0 C1850 2 25 ENDCOMMON 3 0 C1850 2 26 DATA 3 39 C1850 2 27 E-CM DATA-CM DATA-ERR C1850 2 28 MEV MB/SR/MEV MB/SR/MEV C1850 2 29 1.234 5.984E+00 2.496E-01 C1850 2 30 1.310 6.070E+00 3.352E-01 C1850 2 31 1.416 5.735E+00 3.931E-01 C1850 2 32 1.447 5.342E+00 C1850 2 33 1.477 4.975E+00 C1850 2 34 1.568 4.975E+00 C1850 2 35 1.644 5.047E+00 3.459E-01 C1850 2 36 1.705 4.768E+00 1.989E-01 C1850 2 37 1.750 4.701E+00 C1850 2 38 1.826 4.634E+00 1.933E-01 C1850 2 39 1.857 4.317E+00 C1850 2 40 1.902 4.317E+00 2.384E-01 C1850 2 41 1.948 4.137E+00 2.284E-01 C1850 2 42 2.008 3.692E+00 2.039E-01 C1850 2 43 2.039 3.343E+00 2.291E-01 C1850 2 44 2.115 2.860E+00 1.960E-01 C1850 2 45 2.145 2.446E+00 C1850 2 46 2.191 2.122E+00 1.455E-01 C1850 2 47 2.221 1.977E+00 C1850 2 48 2.251 1.841E+00 C1850 2 49 2.297 1.644E+00 C1850 2 50 2.327 1.426E+00 5.947E-02 C1850 2 51 2.358 1.273E+00 C1850 2 52 2.418 1.237E+00 8.480E-02 C1850 2 53 2.464 1.220E+00 8.360E-02 C1850 2 54 2.525 7.212E-01 3.983E-02 C1850 2 55 2.631 5.507E-01 3.041E-02 C1850 2 56 2.737 5.828E-01 C1850 2 57 2.752 9.052E-01 4.999E-02 C1850 2 58 2.783 2.005E+00 C1850 2 59 2.783 3.745E+00 C1850 2 60 2.798 1.027E+01 C1850 2 61 2.843 1.443E+01 C1850 2 62 2.919 1.252E+01 C1850 2 63 2.965 6.610E+00 C1850 2 64 3.026 2.626E+00 C1850 2 65 3.056 6.257E-01 C1850 2 66 3.086 4.204E-01 C1850 2 67 3.147 1.060E-01 C1850 2 68 ENDDATA 41 0 C1850 2 69 ENDSUBENT 68 0 C1850 299999 SUBENT C1850003 20180315 C174C1850 3 1 BIB 5 18 C1850 3 2 REACTION (6-C-12(P,X)2-HE-4,,DA/DE) C1850 3 3 SAMPLE A thin self-supported polystyrene (CH) target located C1850 3 4 at the center of a 1 m diam. scattering chamber. C1850 3 5 Targets of thicknesses ranging from 50 to C1850 3 6 150 microg/cm2 were used. C1850 3 7 DETECTOR (SIBAR) The alpha spectra were measured using a thin C1850 3 8 Ortec Surface Barrier detector (50 microm thickness, C1850 3 9 totally depleted at a reverse bias of about 100 V). C1850 3 10 ERR-ANALYS (DATA-ERR) The absolute differential cross sections C1850 3 11 for the ground state group are accurate to within C1850 3 12 about 25%. The large uncertainty is due to the fact C1850 3 13 that the usual precautions with regard to charge C1850 3 14 collection have not been carefully observed since the C1850 3 15 main emphasis in this experiment was on energy C1850 3 16 spectra. In those cases where the continuous spectra C1850 3 17 are well described by the four-body shape, the C1850 3 18 breakup cross section is accurate to within 25 %. C1850 3 19 STATUS (CURVE) Fig. 1, page 121. C1850 3 20 ENDBIB 18 0 C1850 3 21 COMMON 2 3 C1850 3 22 EN ANG C1850 3 23 MEV ADEG C1850 3 24 14.3 86.0 C1850 3 25 ENDCOMMON 3 0 C1850 3 26 DATA 3 35 C1850 3 27 E-CM DATA-CM DATA-ERR C1850 3 28 MEV MB/SR/MEV MB/SR/MEV C1850 3 29 2.115 6.274E+00 C1850 3 30 2.160 6.013E+00 C1850 3 31 2.236 5.005E+00 C1850 3 32 2.282 3.992E+00 C1850 3 33 2.327 3.010E+00 C1850 3 34 2.403 2.367E+00 C1850 3 35 2.449 2.085E+00 C1850 3 36 2.525 1.862E+00 1.023E-01 C1850 3 37 2.585 1.785E+00 9.804E-02 C1850 3 38 2.646 1.572E+00 8.633E-02 C1850 3 39 2.707 1.572E+00 1.072E-01 C1850 3 40 2.752 1.404E+00 9.571E-02 C1850 3 41 2.813 1.271E+00 5.276E-02 C1850 3 42 2.904 1.136E+00 C1850 3 43 2.965 9.860E-01 5.417E-02 C1850 3 44 3.041 1.043E+00 5.732E-02 C1850 3 45 3.102 7.977E-01 C1850 3 46 3.177 6.829E-01 2.834E-02 C1850 3 47 3.238 7.125E-01 4.859E-02 C1850 3 48 3.284 6.099E-01 4.957E-02 C1850 3 49 3.329 6.186E-01 4.218E-02 C1850 3 50 3.345 4.598E-01 3.737E-02 C1850 3 51 3.420 4.664E-01 3.790E-02 C1850 3 52 3.466 4.470E-01 2.456E-02 C1850 3 53 3.542 4.534E-01 2.491E-02 C1850 3 54 3.603 4.407E-01 2.421E-02 C1850 3 55 3.633 5.604E-01 C1850 3 56 3.739 2.334E+00 C1850 3 57 3.770 4.470E+00 C1850 3 58 3.815 6.829E+00 C1850 3 59 3.876 7.865E+00 C1850 3 60 3.967 4.598E+00 C1850 3 61 4.013 2.026E+00 C1850 3 62 4.073 5.076E-01 C1850 3 63 4.134 7.755E-02 C1850 3 64 ENDDATA 37 0 C1850 3 65 ENDSUBENT 64 0 C1850 399999 SUBENT C1850004 20180315 C174C1850 4 1 BIB 5 18 C1850 4 2 REACTION (6-C-12(P,X)2-HE-4,,DA/DE) C1850 4 3 SAMPLE A thin self-supported polystyrene (CH) target located C1850 4 4 at the center of a 1 m diam. scattering chamber. C1850 4 5 Targets of thicknesses ranging from 50 to C1850 4 6 150 microg/cm2 were used. C1850 4 7 DETECTOR (SIBAR) The alpha spectra were measured using a thin C1850 4 8 Ortec Surface Barrier detector (50 microm thickness, C1850 4 9 totally depleted at a reverse bias of about 100 V). C1850 4 10 ERR-ANALYS (DATA-ERR) The absolute differential cross sections C1850 4 11 for the ground state group are accurate to within C1850 4 12 about 25%. The large uncertainty is due to the fact C1850 4 13 that the usual precautions with regard to charge C1850 4 14 collection have not been carefully observed since the C1850 4 15 main emphasis in this experiment was on energy C1850 4 16 spectra. In those cases where the continuous spectra C1850 4 17 are well described by the four-body shape, the C1850 4 18 breakup cross section is accurate to within 25 %. C1850 4 19 STATUS (CURVE) Fig. 1, page 121. C1850 4 20 ENDBIB 18 0 C1850 4 21 COMMON 2 3 C1850 4 22 EN ANG C1850 4 23 MEV ADEG C1850 4 24 16.0 90.0 C1850 4 25 ENDCOMMON 3 0 C1850 4 26 DATA 3 64 C1850 4 27 E-CM DATA-CM DATA-ERR C1850 4 28 MEV MB/SR/MEV MB/SR/MEV C1850 4 29 2.175 9.047E+00 5.030E-01 C1850 4 30 2.206 8.303E+00 C1850 4 31 2.251 8.069E+00 3.389E-01 C1850 4 32 2.297 7.197E+00 3.023E-01 C1850 4 33 2.342 7.621E+00 4.237E-01 C1850 4 34 2.403 7.301E+00 3.066E-01 C1850 4 35 2.433 6.700E+00 1.889E-01 C1850 4 36 2.494 6.328E+00 3.518E-01 C1850 4 37 2.525 5.725E+00 1.614E-01 C1850 4 38 2.540 5.330E+00 2.963E-01 C1850 4 39 2.570 4.620E+00 3.188E-01 C1850 4 40 2.631 4.554E+00 2.532E-01 C1850 4 41 2.676 4.363E+00 2.426E-01 C1850 4 42 2.722 4.240E+00 2.926E-01 C1850 4 43 2.798 4.240E+00 2.357E-01 C1850 4 44 2.874 4.120E+00 2.291E-01 C1850 4 45 2.919 4.120E+00 2.291E-01 C1850 4 46 2.950 3.728E+00 2.073E-01 C1850 4 47 3.026 3.836E+00 2.133E-01 C1850 4 48 3.071 3.622E+00 2.500E-01 C1850 4 49 3.162 3.781E+00 2.610E-01 C1850 4 50 3.193 4.962E+00 C1850 4 51 3.223 7.301E+00 C1850 4 52 3.269 1.059E+01 C1850 4 53 3.329 1.137E+01 C1850 4 54 3.375 1.044E+01 C1850 4 55 3.420 6.895E+00 C1850 4 56 3.496 3.781E+00 C1850 4 57 3.527 2.498E+00 C1850 4 58 3.618 1.850E+00 C1850 4 59 3.663 1.370E+00 5.753E-02 C1850 4 60 3.724 1.430E+00 C1850 4 61 3.754 1.275E+00 7.090E-02 C1850 4 62 3.800 1.121E+00 3.162E-02 C1850 4 63 3.846 1.257E+00 8.676E-02 C1850 4 64 3.921 1.074E+00 5.972E-02 C1850 4 65 3.937 1.187E+00 6.601E-02 C1850 4 66 3.997 9.178E-01 6.334E-02 C1850 4 67 4.043 9.444E-01 3.966E-02 C1850 4 68 4.058 1.074E+00 5.972E-02 C1850 4 69 4.119 9.718E-01 2.740E-02 C1850 4 70 4.180 8.303E-01 6.828E-02 C1850 4 71 4.225 9.047E-01 5.030E-02 C1850 4 72 4.256 7.621E-01 4.237E-02 C1850 4 73 4.316 7.955E-01 6.541E-02 C1850 4 74 4.347 6.895E-01 C1850 4 75 4.423 6.328E-01 1.784E-02 C1850 4 76 4.423 6.994E-01 3.889E-02 C1850 4 77 4.468 6.062E-01 C1850 4 78 4.514 5.976E-01 4.914E-02 C1850 4 79 4.574 5.807E-01 4.008E-02 C1850 4 80 4.635 5.725E-01 3.183E-02 C1850 4 81 4.681 4.822E-01 3.328E-02 C1850 4 82 4.757 5.563E-01 C1850 4 83 4.757 4.822E-01 3.328E-02 C1850 4 84 4.817 9.718E-01 C1850 4 85 4.863 2.721E+00 C1850 4 86 4.893 7.301E+00 C1850 4 87 4.939 9.718E+00 C1850 4 88 4.969 1.029E+01 C1850 4 89 5.000 1.059E+01 C1850 4 90 5.045 6.895E+00 C1850 4 91 5.091 2.761E+00 C1850 4 92 5.136 5.254E-01 C1850 4 93 ENDDATA 66 0 C1850 4 94 ENDSUBENT 93 0 C1850 499999 SUBENT C1850005 20180315 C174C1850 5 1 BIB 5 18 C1850 5 2 REACTION (6-C-12(P,X)2-HE-4,,DA/DE) C1850 5 3 SAMPLE A thin self-supported polystyrene (CH) target located C1850 5 4 at the center of a 1 m diam. scattering chamber. C1850 5 5 Targets of thicknesses ranging from 50 to C1850 5 6 150 microg/cm2 were used. C1850 5 7 DETECTOR (SIBAR) The alpha spectra were measured using a thin C1850 5 8 Ortec Surface Barrier detector (50 microm thickness, C1850 5 9 totally depleted at a reverse bias of about 100 V). C1850 5 10 ERR-ANALYS (DATA-ERR) The absolute differential cross sections C1850 5 11 for the ground state group are accurate to within C1850 5 12 about 25%. The large uncertainty is due to the fact C1850 5 13 that the usual precautions with regard to charge C1850 5 14 collection have not been carefully observed since the C1850 5 15 main emphasis in this experiment was on energy C1850 5 16 spectra. In those cases where the continuous spectra C1850 5 17 are well described by the four-body shape, the C1850 5 18 breakup cross section is accurate to within 25 %. C1850 5 19 STATUS (CURVE) Fig. 1, page 121. C1850 5 20 ENDBIB 18 0 C1850 5 21 COMMON 2 3 C1850 5 22 EN ANG C1850 5 23 MEV ADEG C1850 5 24 18.3 90.0 C1850 5 25 ENDCOMMON 3 0 C1850 5 26 DATA 3 57 C1850 5 27 E-CM DATA-CM DATA-ERR C1850 5 28 MEV MB/SR/MEV MB/SR/MEV C1850 5 29 3.679 5.148E+00 C1850 5 30 3.694 5.371E+00 4.751E-01 C1850 5 31 3.770 5.296E+00 3.611E-01 C1850 5 32 3.876 4.598E+00 3.136E-01 C1850 5 33 3.937 4.407E+00 3.006E-01 C1850 5 34 3.982 3.827E+00 1.588E-01 C1850 5 35 4.028 3.881E+00 2.132E-01 C1850 5 36 4.089 3.827E+00 3.110E-01 C1850 5 37 4.134 3.720E+00 2.044E-01 C1850 5 38 4.210 3.773E+00 2.573E-01 C1850 5 39 4.256 3.566E+00 C1850 5 40 4.301 3.566E+00 2.432E-01 C1850 5 41 4.347 3.096E+00 1.701E-01 C1850 5 42 4.377 3.276E+00 1.800E-01 C1850 5 43 4.453 3.096E+00 2.111E-01 C1850 5 44 4.529 3.466E+00 1.904E-01 C1850 5 45 4.650 3.185E+00 2.172E-01 C1850 5 46 4.726 4.470E+00 C1850 5 47 4.772 5.683E+00 C1850 5 48 4.832 6.546E+00 C1850 5 49 4.863 7.125E+00 C1850 5 50 4.908 6.926E+00 C1850 5 51 4.924 6.274E+00 C1850 5 52 4.984 4.797E+00 C1850 5 53 5.030 3.773E+00 C1850 5 54 5.091 2.175E+00 C1850 5 55 5.121 1.345E+00 C1850 5 56 5.151 1.058E+00 C1850 5 57 5.197 6.639E-01 5.395E-02 C1850 5 58 5.258 6.274E-01 3.447E-02 C1850 5 59 5.288 5.846E-01 8.200E-03 C1850 5 60 5.334 7.025E-01 4.790E-02 C1850 5 61 5.379 5.296E-01 C1850 5 62 5.425 4.935E-01 3.365E-02 C1850 5 63 5.501 5.148E-01 C1850 5 64 5.516 4.470E-01 2.456E-02 C1850 5 65 5.561 4.730E-01 3.844E-02 C1850 5 66 5.607 4.165E-01 2.840E-02 C1850 5 67 5.713 4.470E-01 2.456E-02 C1850 5 68 5.744 3.185E-01 2.172E-02 C1850 5 69 5.850 2.144E-01 1.462E-02 C1850 5 70 5.865 3.185E-01 2.172E-02 C1850 5 71 5.971 2.470E-01 1.684E-02 C1850 5 72 6.062 1.942E-01 1.325E-02 C1850 5 73 6.108 3.370E-01 2.298E-02 C1850 5 74 6.199 3.010E-01 C1850 5 75 6.245 6.829E-01 C1850 5 76 6.305 1.862E+00 C1850 5 77 6.351 3.140E+00 C1850 5 78 6.381 4.663E+00 C1850 5 79 6.396 5.604E+00 C1850 5 80 6.472 6.639E+00 C1850 5 81 6.609 6.099E+00 C1850 5 82 6.655 3.881E+00 C1850 5 83 6.700 1.345E+00 C1850 5 84 6.700 4.165E-01 C1850 5 85 6.791 5.764E-02 C1850 5 86 ENDDATA 59 0 C1850 5 87 ENDSUBENT 86 0 C1850 599999 SUBENT C1850006 20180315 C174C1850 6 1 BIB 4 9 C1850 6 2 REACTION (6-C-12(P,X)2-HE-4,,DA/DE) C1850 6 3 SAMPLE A thin self-supported polystyrene (CH) target located C1850 6 4 at the center of a 1 m diam. scattering chamber. C1850 6 5 Targets of thicknesses ranging from 50 to C1850 6 6 150 microg/cm2 were used. C1850 6 7 DETECTOR (SIBAR) The alpha spectra were measured using a thin C1850 6 8 Ortec Surface Barrier detector (50 microm thickness, C1850 6 9 totally depleted at a reverse bias of about 100 V). C1850 6 10 STATUS (CURVE) Fig. 2, page 122. C1850 6 11 ENDBIB 9 0 C1850 6 12 COMMON 2 3 C1850 6 13 EN ANG C1850 6 14 MEV ADEG C1850 6 15 14.3 41.0 C1850 6 16 ENDCOMMON 3 0 C1850 6 17 DATA 2 87 C1850 6 18 E-CM DATA-CM C1850 6 19 MEV MB/SR/MEV C1850 6 20 1.431 4.587E+00 C1850 6 21 1.475 5.038E+00 C1850 6 22 1.487 4.430E+00 C1850 6 23 1.537 4.329E+00 C1850 6 24 1.581 4.279E+00 C1850 6 25 1.612 4.645E+00 C1850 6 26 1.655 4.592E+00 C1850 6 27 1.674 4.812E+00 C1850 6 28 1.686 4.647E+00 C1850 6 29 1.730 4.870E+00 C1850 6 30 1.730 4.332E+00 C1850 6 31 1.780 4.929E+00 C1850 6 32 1.805 4.704E+00 C1850 6 33 1.836 4.760E+00 C1850 6 34 1.873 4.651E+00 C1850 6 35 1.873 4.285E+00 C1850 6 36 1.898 4.651E+00 C1850 6 37 1.911 4.762E+00 C1850 6 38 1.954 4.492E+00 C1850 6 39 1.985 4.440E+00 C1850 6 40 2.023 4.288E+00 C1850 6 41 2.035 4.654E+00 C1850 6 42 2.041 4.189E+00 C1850 6 43 2.079 3.998E+00 C1850 6 44 2.110 4.656E+00 C1850 6 45 2.147 4.767E+00 C1850 6 46 2.160 4.995E+00 C1850 6 47 2.172 5.682E+00 C1850 6 48 2.172 5.359E+00 C1850 6 49 2.190 6.096E+00 C1850 6 50 2.209 6.539E+00 C1850 6 51 2.240 6.934E+00 C1850 6 52 2.278 6.542E+00 C1850 6 53 2.290 6.170E+00 C1850 6 54 2.296 5.888E+00 C1850 6 55 2.309 5.619E+00 C1850 6 56 2.321 5.239E+00 C1850 6 57 2.334 4.941E+00 C1850 6 58 2.346 4.500E+00 C1850 6 59 2.353 3.957E+00 C1850 6 60 2.372 3.646E+00 C1850 6 61 2.384 3.480E+00 C1850 6 62 2.384 3.282E+00 C1850 6 63 2.397 3.096E+00 C1850 6 64 2.409 2.819E+00 C1850 6 65 2.435 2.366E+00 C1850 6 66 2.472 2.232E+00 C1850 6 67 2.522 1.963E+00 C1850 6 68 2.547 1.726E+00 C1850 6 69 2.597 1.767E+00 C1850 6 70 2.628 1.609E+00 C1850 6 71 2.684 1.610E+00 C1850 6 72 2.715 1.501E+00 C1850 6 73 2.765 1.450E+00 C1850 6 74 2.796 1.688E+00 C1850 6 75 2.840 1.433E+00 C1850 6 76 2.884 1.275E+00 C1850 6 77 2.927 1.417E+00 C1850 6 78 2.971 1.451E+00 C1850 6 79 3.002 1.122E+00 C1850 6 80 3.039 1.176E+00 C1850 6 81 3.096 1.084E+00 C1850 6 82 3.133 1.084E+00 C1850 6 83 3.177 8.579E-01 C1850 6 84 3.214 9.204E-01 C1850 6 85 3.264 6.952E-01 C1850 6 86 3.289 6.872E-01 C1850 6 87 3.345 6.955E-01 C1850 6 88 3.383 6.335E-01 C1850 6 89 3.433 6.118E-01 C1850 6 90 3.477 4.675E-01 C1850 6 91 3.514 4.515E-01 C1850 6 92 3.539 3.745E-01 C1850 6 93 3.639 3.617E-01 C1850 6 94 3.689 3.576E-01 C1850 6 95 3.701 3.704E-01 C1850 6 96 3.726 4.020E-01 C1850 6 97 3.762 8.909E-01 C1850 6 98 3.798 3.008E+00 C1850 6 99 3.847 6.363E+00 C1850 6 100 3.896 8.627E+00 C1850 6 101 3.946 7.766E+00 C1850 6 102 3.978 5.157E+00 C1850 6 103 4.028 2.711E+00 C1850 6 104 4.055 9.683E-01 C1850 6 105 4.094 2.351E-01 C1850 6 106 4.158 8.110E-02 C1850 6 107 ENDDATA 89 0 C1850 6 108 ENDSUBENT 107 0 C1850 699999 SUBENT C1850007 20180315 C174C1850 7 1 BIB 5 18 C1850 7 2 REACTION (6-C-12(P,X)2-HE-4,,DA/DE) C1850 7 3 SAMPLE A thin self-supported polystyrene (CH) target located C1850 7 4 at the center of a 1 m diam. scattering chamber. C1850 7 5 Targets of thicknesses ranging from 50 to C1850 7 6 150 microg/cm2 were used. C1850 7 7 DETECTOR (SIBAR) The alpha spectra were measured using a thin C1850 7 8 Ortec Surface Barrier detector (50 microm thickness, C1850 7 9 totally depleted at a reverse bias of about 100 V). C1850 7 10 ERR-ANALYS (DATA-ERR) The absolute differential cross sections C1850 7 11 for the ground state group are accurate to within C1850 7 12 about 25%. The large uncertainty is due to the fact C1850 7 13 that the usual precautions with regard to charge C1850 7 14 collection have not been carefully observed since the C1850 7 15 main emphasis in this experiment was on energy C1850 7 16 spectra. In those cases where the continuous spectra C1850 7 17 are well described by the four-body shape, the C1850 7 18 breakup cross section is accurate to within 25 %. C1850 7 19 STATUS (CURVE) Fig. 3, page 123. C1850 7 20 ENDBIB 18 0 C1850 7 21 COMMON 2 3 C1850 7 22 EN ANG C1850 7 23 MEV ADEG C1850 7 24 16.0 22.0 C1850 7 25 ENDCOMMON 3 0 C1850 7 26 DATA 3 84 C1850 7 27 E-CM DATA-CM DATA-ERR C1850 7 28 MEV MB/SR/MEV MB/SR/MEV C1850 7 29 2.093 9.981E+00 7.492E-01 C1850 7 30 2.115 9.363E+00 5.791E-01 C1850 7 31 2.153 9.633E+00 4.014E-01 C1850 7 32 2.183 8.722E+00 4.812E-01 C1850 7 33 2.235 8.359E+00 4.049E-01 C1850 7 34 2.280 8.183E+00 4.514E-01 C1850 7 35 2.288 9.166E+00 4.440E-01 C1850 7 36 2.355 8.910E+00 3.713E-01 C1850 7 37 2.385 8.538E+00 4.711E-01 C1850 7 38 2.438 7.462E+00 5.110E-01 C1850 7 39 2.490 7.568E+00 5.183E-01 C1850 7 40 2.543 7.409E+00 4.582E-01 C1850 7 41 2.580 6.804E+00 5.108E-01 C1850 7 42 2.655 6.614E+00 4.529E-01 C1850 7 43 2.685 5.989E+00 3.704E-01 C1850 7 44 2.745 6.031E+00 4.130E-01 C1850 7 45 2.775 5.234E+00 2.887E-01 C1850 7 46 2.820 5.946E+00 4.072E-01 C1850 7 47 2.858 6.031E+00 3.730E-01 C1850 7 48 2.880 5.271E+00 3.260E-01 C1850 7 49 2.918 5.346E+00 3.661E-01 C1850 7 50 2.963 4.980E+00 3.080E-01 C1850 7 51 3.008 5.087E+00 2.807E-01 C1850 7 52 3.068 4.773E+00 2.952E-01 C1850 7 53 3.113 4.807E+00 3.292E-01 C1850 7 54 3.165 4.807E+00 2.973E-01 C1850 7 55 3.218 4.739E+00 2.931E-01 C1850 7 56 3.248 5.051E+00 C1850 7 57 3.293 5.234E+00 C1850 7 58 3.293 5.500E+00 C1850 7 59 3.345 5.780E+00 C1850 7 60 3.368 6.338E+00 C1850 7 61 3.375 6.661E+00 C1850 7 62 3.390 7.202E+00 C1850 7 63 3.405 7.622E+00 C1850 7 64 3.450 7.151E+00 C1850 7 65 3.465 6.521E+00 C1850 7 66 3.503 5.821E+00 C1850 7 67 3.510 5.016E+00 C1850 7 68 3.518 5.308E+00 2.572E-01 C1850 7 69 3.548 4.672E+00 C1850 7 70 3.563 4.291E+00 2.654E-01 C1850 7 71 3.578 3.568E+00 2.678E-01 C1850 7 72 3.593 2.172E+00 1.198E-01 C1850 7 73 3.600 3.074E+00 C1850 7 74 3.660 2.298E+00 1.268E-01 C1850 7 75 3.735 1.939E+00 9.391E-02 C1850 7 76 3.765 2.009E+00 1.108E-01 C1850 7 77 3.825 1.980E+00 1.225E-01 C1850 7 78 3.893 1.743E+00 9.616E-02 C1850 7 79 3.900 1.429E+00 7.884E-02 C1850 7 80 3.953 1.635E+00 1.011E-01 C1850 7 81 4.013 1.601E+00 9.900E-02 C1850 7 82 4.073 1.491E+00 8.226E-02 C1850 7 83 4.125 1.341E+00 7.396E-02 C1850 7 84 4.178 1.360E+00 8.410E-02 C1850 7 85 4.230 1.084E+00 7.420E-02 C1850 7 86 4.283 1.017E+00 6.962E-02 C1850 7 87 4.313 1.053E+00 8.595E-02 C1850 7 88 4.373 1.009E+00 7.577E-02 C1850 7 89 4.410 9.952E-01 9.408E-02 C1850 7 90 4.440 8.884E-01 5.495E-02 C1850 7 91 4.478 7.600E-01 4.701E-02 C1850 7 92 4.508 6.410E-01 3.537E-02 C1850 7 93 4.523 8.217E-01 5.627E-02 C1850 7 94 4.568 7.232E-01 4.473E-02 C1850 7 95 4.620 6.785E-01 4.646E-02 C1850 7 96 4.635 6.057E-01 4.148E-02 C1850 7 97 4.673 5.109E-01 2.818E-02 C1850 7 98 4.733 4.692E-01 3.829E-02 C1850 7 99 4.733 5.763E-01 5.449E-02 C1850 7 100 4.808 4.593E-01 4.046E-02 C1850 7 101 4.830 6.143E-01 C1850 7 102 4.883 9.811E-01 C1850 7 103 4.913 2.081E+00 C1850 7 104 4.965 5.123E+00 C1850 7 105 4.973 8.784E+00 C1850 7 106 5.040 1.235E+01 C1850 7 107 5.123 9.101E+00 C1850 7 108 5.168 5.618E+00 C1850 7 109 5.198 2.485E+00 C1850 7 110 5.228 1.214E+00 C1850 7 111 5.280 3.508E-01 C1850 7 112 5.317 1.254E-01 C1850 7 113 ENDDATA 86 0 C1850 7 114 ENDSUBENT 113 0 C1850 799999 SUBENT C1850008 20180315 C174C1850 8 1 BIB 5 18 C1850 8 2 REACTION (6-C-12(P,X)2-HE-4,,DA/DE) C1850 8 3 SAMPLE A thin self-supported polystyrene (CH) target located C1850 8 4 at the center of a 1 m diam. scattering chamber. C1850 8 5 Targets of thicknesses ranging from 50 to C1850 8 6 150 microg/cm2 were used. C1850 8 7 DETECTOR (SIBAR) The alpha spectra were measured using a thin C1850 8 8 Ortec Surface Barrier detector (50 microm thickness, C1850 8 9 totally depleted at a reverse bias of about 100 V). C1850 8 10 ERR-ANALYS (DATA-ERR) The absolute differential cross sections C1850 8 11 for the ground state group are accurate to within C1850 8 12 about 25%. The large uncertainty is due to the fact C1850 8 13 that the usual precautions with regard to charge C1850 8 14 collection have not been carefully observed since the C1850 8 15 main emphasis in this experiment was on energy C1850 8 16 spectra. In those cases where the continuous spectra C1850 8 17 are well described by the four-body shape, the C1850 8 18 breakup cross section is accurate to within 25 %. C1850 8 19 STATUS (CURVE) Fig. 3, page 123. C1850 8 20 ENDBIB 18 0 C1850 8 21 COMMON 2 3 C1850 8 22 EN ANG C1850 8 23 MEV ADEG C1850 8 24 16.0 30.0 C1850 8 25 ENDCOMMON 3 0 C1850 8 26 DATA 3 78 C1850 8 27 E-CM DATA-CM DATA-ERR C1850 8 28 MEV MB/SR/MEV MB/SR/MEV C1850 8 29 1.894 8.781E+00 4.746E-01 C1850 8 30 1.937 9.357E+00 5.757E-01 C1850 8 31 1.987 9.507E+00 7.255E-01 C1850 8 32 2.072 9.065E+00 5.578E-01 C1850 8 33 2.123 9.283E+00 8.435E-01 C1850 8 34 2.157 8.440E+00 5.819E-01 C1850 8 35 2.199 8.440E+00 5.193E-01 C1850 8 36 2.250 8.440E+00 6.440E-01 C1850 8 37 2.292 8.440E+00 5.193E-01 C1850 8 38 2.368 8.373E+00 5.152E-01 C1850 8 39 2.444 7.552E+00 4.647E-01 C1850 8 40 2.495 7.316E+00 4.502E-01 C1850 8 41 2.537 6.651E+00 4.093E-01 C1850 8 42 2.580 6.292E+00 4.801E-01 C1850 8 43 2.597 5.812E+00 3.576E-01 C1850 8 44 2.647 5.675E+00 3.067E-01 C1850 8 45 2.681 6.443E+00 2.997E-01 C1850 8 46 2.698 6.047E+00 2.813E-01 C1850 8 47 2.732 5.242E+00 3.225E-01 C1850 8 48 2.791 5.242E+00 3.225E-01 C1850 8 49 2.859 4.998E+00 3.075E-01 C1850 8 50 2.918 4.766E+00 4.330E-01 C1850 8 51 2.952 4.617E+00 2.841E-01 C1850 8 52 2.994 4.617E+00 3.523E-01 C1850 8 53 3.045 4.728E+00 3.260E-01 C1850 8 54 3.079 4.544E+00 2.796E-01 C1850 8 55 3.087 3.908E+00 2.112E-01 C1850 8 56 3.130 4.098E+00 2.826E-01 C1850 8 57 3.181 4.066E+00 3.400E-01 C1850 8 58 3.248 4.034E+00 1.876E-01 C1850 8 59 3.274 4.919E+00 3.392E-01 C1850 8 60 3.316 6.047E+00 4.169E-01 C1850 8 61 3.341 7.087E+00 6.440E-01 C1850 8 62 3.401 7.433E+00 4.574E-01 C1850 8 63 3.451 7.433E+00 3.457E-01 C1850 8 64 3.468 5.497E+00 3.791E-01 C1850 8 65 3.502 4.333E+00 3.306E-01 C1850 8 66 3.544 3.414E+00 2.855E-01 C1850 8 67 3.587 2.486E+00 1.714E-01 C1850 8 68 3.604 2.296E+00 8.934E-02 C1850 8 69 3.646 1.824E+00 1.257E-01 C1850 8 70 3.688 1.685E+00 1.409E-01 C1850 8 71 3.714 1.619E+00 1.236E-01 C1850 8 72 3.764 1.556E+00 1.301E-01 C1850 8 73 3.798 1.349E+00 8.299E-02 C1850 8 74 3.832 1.472E+00 7.956E-02 C1850 8 75 3.866 1.403E+00 9.677E-02 C1850 8 76 3.934 1.286E+00 1.075E-01 C1850 8 77 4.010 1.055E+00 8.048E-02 C1850 8 78 4.086 1.046E+00 6.438E-02 C1850 8 79 4.162 1.055E+00 1.331E-01 C1850 8 80 4.196 8.856E-01 7.405E-02 C1850 8 81 4.238 8.927E-01 6.155E-02 C1850 8 82 4.289 9.070E-01 6.254E-02 C1850 8 83 4.357 7.738E-01 5.905E-02 C1850 8 84 4.399 8.311E-01 8.149E-02 C1850 8 85 4.416 7.148E-01 7.008E-02 C1850 8 86 4.475 7.556E-01 7.948E-02 C1850 8 87 4.560 6.655E-01 5.078E-02 C1850 8 88 4.585 7.320E-01 5.047E-02 C1850 8 89 4.619 6.245E-01 6.124E-02 C1850 8 90 4.653 5.633E-01 4.710E-02 C1850 8 91 4.695 5.286E-01 5.560E-02 C1850 8 92 4.755 4.267E-01 2.942E-02 C1850 8 93 4.805 4.656E-01 3.553E-02 C1850 8 94 4.848 4.922E-01 3.756E-02 C1850 8 95 4.890 5.861E-01 C1850 8 96 4.915 1.685E+00 C1850 8 97 4.932 3.667E+00 C1850 8 98 4.983 7.087E+00 C1850 8 99 5.017 1.005E+01 C1850 8 100 5.051 1.187E+01 C1850 8 101 5.085 9.357E+00 C1850 8 102 5.152 5.812E+00 C1850 8 103 5.186 2.913E+00 C1850 8 104 5.229 1.328E+00 C1850 8 105 5.245 6.396E-01 C1850 8 106 5.305 2.088E-01 C1850 8 107 ENDDATA 80 0 C1850 8 108 ENDSUBENT 107 0 C1850 899999 SUBENT C1850009 20180315 C174C1850 9 1 BIB 5 18 C1850 9 2 REACTION (6-C-12(P,X)2-HE-4,,DA/DE) C1850 9 3 SAMPLE A thin self-supported polystyrene (CH) target located C1850 9 4 at the center of a 1 m diam. scattering chamber. C1850 9 5 Targets of thicknesses ranging from 50 to C1850 9 6 150 microg/cm2 were used. C1850 9 7 DETECTOR (SIBAR) The alpha spectra were measured using a thin C1850 9 8 Ortec Surface Barrier detector (50 microm thickness, C1850 9 9 totally depleted at a reverse bias of about 100 V). C1850 9 10 ERR-ANALYS (DATA-ERR) The absolute differential cross sections C1850 9 11 for the ground state group are accurate to within C1850 9 12 about 25%. The large uncertainty is due to the fact C1850 9 13 that the usual precautions with regard to charge C1850 9 14 collection have not been carefully observed since the C1850 9 15 main emphasis in this experiment was on energy C1850 9 16 spectra. In those cases where the continuous spectra C1850 9 17 are well described by the four-body shape, the C1850 9 18 breakup cross section is accurate to within 25 %. C1850 9 19 STATUS (CURVE) Fig. 3, page 123. C1850 9 20 ENDBIB 18 0 C1850 9 21 COMMON 2 3 C1850 9 22 EN ANG C1850 9 23 MEV ADEG C1850 9 24 16.0 60.0 C1850 9 25 ENDCOMMON 3 0 C1850 9 26 DATA 3 74 C1850 9 27 E-CM DATA-CM DATA-ERR C1850 9 28 MEV MB/SR/MEV MB/SR/MEV C1850 9 29 1.717 1.019E+01 6.612E-01 C1850 9 30 1.748 1.039E+01 5.804E-01 C1850 9 31 1.778 9.262E+00 4.332E-01 C1850 9 32 1.840 9.174E+00 5.124E-01 C1850 9 33 1.881 8.914E+00 5.782E-01 C1850 9 34 1.932 8.100E+00 4.524E-01 C1850 9 35 1.993 7.870E+00 6.501E-01 C1850 9 36 2.044 7.946E+00 6.564E-01 C1850 9 37 2.095 8.178E+00 6.755E-01 C1850 9 38 2.136 8.022E+00 4.481E-01 C1850 9 39 2.218 7.721E+00 4.313E-01 C1850 9 40 2.258 7.431E+00 4.151E-01 C1850 9 41 2.289 7.016E+00 4.550E-01 C1850 9 42 2.320 6.687E+00 4.338E-01 C1850 9 43 2.371 6.752E+00 3.771E-01 C1850 9 44 2.412 7.083E+00 6.471E-01 C1850 9 45 2.452 6.624E+00 4.296E-01 C1850 9 46 2.483 6.882E+00 3.844E-01 C1850 9 47 2.524 6.752E+00 4.379E-01 C1850 9 48 2.555 6.498E+00 4.215E-01 C1850 9 49 2.585 6.194E+00 3.460E-01 C1850 9 50 2.626 5.904E+00 4.877E-01 C1850 9 51 2.657 5.469E+00 3.547E-01 C1850 9 52 2.687 5.114E+00 3.773E-01 C1850 9 53 2.759 5.469E+00 4.518E-01 C1850 9 54 2.810 5.213E+00 3.846E-01 C1850 9 55 2.851 4.782E+00 3.951E-01 C1850 9 56 2.871 4.345E+00 2.427E-01 C1850 9 57 2.943 4.429E+00 3.268E-01 C1850 9 58 3.004 4.647E+00 3.428E-01 C1850 9 59 3.065 4.782E+00 3.102E-01 C1850 9 60 3.106 4.304E+00 2.792E-01 C1850 9 61 3.157 4.472E+00 3.299E-01 C1850 9 62 3.188 4.142E+00 2.314E-01 C1850 9 63 3.229 4.603E+00 2.571E-01 C1850 9 64 3.269 6.019E+00 5.498E-01 C1850 9 65 3.300 8.416E+00 5.459E-01 C1850 9 66 3.361 1.133E+01 6.327E-01 C1850 9 67 3.412 1.235E+01 8.008E-01 C1850 9 68 3.453 1.122E+01 9.267E-01 C1850 9 69 3.474 7.946E+00 5.862E-01 C1850 9 70 3.515 5.065E+00 3.285E-01 C1850 9 71 3.555 3.229E+00 2.382E-01 C1850 9 72 3.586 2.422E+00 1.571E-01 C1850 9 73 3.586 1.888E+00 1.055E-01 C1850 9 74 3.668 1.651E+00 7.723E-02 C1850 9 75 3.698 1.417E+00 1.170E-01 C1850 9 76 3.749 1.300E+00 7.259E-02 C1850 9 77 3.801 1.083E+00 7.026E-02 C1850 9 78 3.862 8.608E-01 7.111E-02 C1850 9 79 3.913 1.023E+00 5.713E-02 C1850 9 80 3.964 7.600E-01 4.929E-02 C1850 9 81 3.974 9.030E-01 7.460E-02 C1850 9 82 4.015 7.314E-01 6.042E-02 C1850 9 83 4.087 6.906E-01 4.479E-02 C1850 9 84 4.087 5.487E-01 4.048E-02 C1850 9 85 4.127 6.215E-01 5.678E-02 C1850 9 86 4.178 5.435E-01 4.965E-02 C1850 9 87 4.209 4.753E-01 3.506E-02 C1850 9 88 4.250 4.402E-01 2.855E-02 C1850 9 89 4.464 3.887E-01 C1850 9 90 4.832 7.245E-01 C1850 9 91 4.853 1.033E+00 C1850 9 92 4.904 3.198E+00 C1850 9 93 4.944 8.336E+00 C1850 9 94 4.995 1.760E+01 C1850 9 95 5.016 2.657E+01 C1850 9 96 5.067 2.761E+01 C1850 9 97 5.118 1.974E+01 C1850 9 98 5.159 1.029E+01 C1850 9 99 5.190 3.355E+00 C1850 9 100 5.230 1.083E+00 C1850 9 101 5.261 3.887E-01 C1850 9 102 5.312 1.859E-01 C1850 9 103 ENDDATA 76 0 C1850 9 104 ENDSUBENT 103 0 C1850 999999 SUBENT C1850010 20180315 C174C1850 10 1 BIB 5 18 C1850 10 2 REACTION (6-C-12(P,X)2-HE-4,,DA/DE) C1850 10 3 SAMPLE A thin self-supported polystyrene (CH) target located C1850 10 4 at the center of a 1 m diam. scattering chamber. C1850 10 5 Targets of thicknesses ranging from 50 to C1850 10 6 150 microg/cm2 were used. C1850 10 7 DETECTOR (SIBAR) The alpha spectra were measured using a thin C1850 10 8 Ortec Surface Barrier detector (50 microm thickness, C1850 10 9 totally depleted at a reverse bias of about 100 V). C1850 10 10 ERR-ANALYS (DATA-ERR) The absolute differential cross sections C1850 10 11 for the ground state group are accurate to within C1850 10 12 about 25%. The large uncertainty is due to the fact C1850 10 13 that the usual precautions with regard to charge C1850 10 14 collection have not been carefully observed since the C1850 10 15 main emphasis in this experiment was on energy C1850 10 16 spectra. In those cases where the continuous spectra C1850 10 17 are well described by the four-body shape, the C1850 10 18 breakup cross section is accurate to within 25 %. C1850 10 19 STATUS (CURVE) Fig. 3, page 123. C1850 10 20 ENDBIB 18 0 C1850 10 21 COMMON 2 3 C1850 10 22 EN ANG C1850 10 23 MEV ADEG C1850 10 24 16.0 90.0 C1850 10 25 ENDCOMMON 3 0 C1850 10 26 DATA 3 67 C1850 10 27 E-CM DATA-CM DATA-ERR C1850 10 28 MEV MB/SR/MEV MB/SR/MEV C1850 10 29 2.289 8.752E+00 4.861E-01 C1850 10 30 2.361 8.587E+00 4.769E-01 C1850 10 31 2.412 7.659E+00 4.254E-01 C1850 10 32 2.422 8.345E+00 4.635E-01 C1850 10 33 2.483 7.587E+00 4.214E-01 C1850 10 34 2.524 7.098E+00 3.300E-01 C1850 10 35 2.585 6.640E+00 4.282E-01 C1850 10 36 2.636 5.594E+00 4.103E-01 C1850 10 37 2.687 4.990E+00 2.771E-01 C1850 10 38 2.728 4.990E+00 3.660E-01 C1850 10 39 2.769 4.624E+00 2.982E-01 C1850 10 40 2.820 4.409E+00 2.843E-01 C1850 10 41 2.861 4.536E+00 2.926E-01 C1850 10 42 2.902 4.409E+00 3.234E-01 C1850 10 43 2.953 4.367E+00 2.816E-01 C1850 10 44 3.004 4.451E+00 2.870E-01 C1850 10 45 3.075 3.575E+00 1.663E-01 C1850 10 46 3.106 4.047E+00 3.324E-01 C1850 10 47 3.157 3.858E+00 3.169E-01 C1850 10 48 3.198 3.714E+00 2.063E-01 C1850 10 49 3.239 3.933E+00 C1850 10 50 3.300 5.134E+00 C1850 10 51 3.310 7.165E+00 C1850 10 52 3.372 1.019E+01 C1850 10 53 3.433 1.121E+01 C1850 10 54 3.464 1.010E+01 C1850 10 55 3.515 6.767E+00 C1850 10 56 3.555 3.714E+00 C1850 10 57 3.607 2.586E+00 C1850 10 58 3.637 2.019E+00 C1850 10 59 3.709 1.353E+00 1.112E-01 C1850 10 60 3.790 1.475E+00 1.082E-01 C1850 10 61 3.811 1.278E+00 1.050E-01 C1850 10 62 3.882 1.129E+00 7.284E-02 C1850 10 63 3.933 1.254E+00 1.139E-01 C1850 10 64 3.964 1.077E+00 7.900E-02 C1850 10 65 3.984 1.242E+00 8.012E-02 C1850 10 66 4.025 1.108E+00 C1850 10 67 4.076 1.067E+00 C1850 10 68 4.087 9.247E-01 5.964E-02 C1850 10 69 4.117 9.698E-01 5.386E-02 C1850 10 70 4.148 1.129E+00 9.277E-02 C1850 10 71 4.189 9.791E-01 7.182E-02 C1850 10 72 4.250 8.407E-01 5.422E-02 C1850 10 73 4.301 8.987E-01 7.382E-02 C1850 10 74 4.403 8.093E-01 7.352E-02 C1850 10 75 4.434 7.016E-01 5.763E-02 C1850 10 76 4.495 6.563E-01 4.815E-02 C1850 10 77 4.546 5.855E-01 4.295E-02 C1850 10 78 4.597 6.024E-01 5.472E-02 C1850 10 79 4.658 5.911E-01 5.369E-02 C1850 10 80 4.699 5.636E-01 4.629E-02 C1850 10 81 4.771 4.748E-01 C1850 10 82 4.832 4.886E-01 C1850 10 83 4.842 5.799E-01 C1850 10 84 4.893 9.885E-01 C1850 10 85 4.955 2.791E+00 C1850 10 86 4.975 7.165E+00 C1850 10 87 5.036 9.905E+00 C1850 10 88 5.057 1.059E+01 C1850 10 89 5.108 1.059E+01 C1850 10 90 5.138 6.832E+00 C1850 10 91 5.149 2.739E+00 C1850 10 92 5.179 1.547E+00 C1850 10 93 5.179 8.734E-01 C1850 10 94 5.220 5.425E-01 C1850 10 95 5.261 1.106E-01 C1850 10 96 ENDDATA 69 0 C1850 10 97 ENDSUBENT 96 0 C1850 1099999 SUBENT C1850011 20180315 C174C1850 11 1 BIB 5 18 C1850 11 2 REACTION (6-C-12(P,X)2-HE-4,,DA/DE) C1850 11 3 SAMPLE A thin self-supported polystyrene (CH) target located C1850 11 4 at the center of a 1 m diam. scattering chamber. C1850 11 5 Targets of thicknesses ranging from 50 to C1850 11 6 150 microg/cm2 were used. C1850 11 7 DETECTOR (SIBAR) The alpha spectra were measured using a thin C1850 11 8 Ortec Surface Barrier detector (50 microm thickness, C1850 11 9 totally depleted at a reverse bias of about 100 V). C1850 11 10 ERR-ANALYS (DATA-ERR) The absolute differential cross sections C1850 11 11 for the ground state group are accurate to within C1850 11 12 about 25%. The large uncertainty is due to the fact C1850 11 13 that the usual precautions with regard to charge C1850 11 14 collection have not been carefully observed since the C1850 11 15 main emphasis in this experiment was on energy C1850 11 16 spectra. In those cases where the continuous spectra C1850 11 17 are well described by the four-body shape, the C1850 11 18 breakup cross section is accurate to within 25 %. C1850 11 19 STATUS (CURVE) Fig. 3, page 123. C1850 11 20 ENDBIB 18 0 C1850 11 21 COMMON 2 3 C1850 11 22 EN ANG C1850 11 23 MEV ADEG C1850 11 24 16.0 120.0 C1850 11 25 ENDCOMMON 3 0 C1850 11 26 DATA 3 30 C1850 11 27 E-CM DATA-CM DATA-ERR C1850 11 28 MEV MB/SR/MEV MB/SR/MEV C1850 11 29 3.617 1.699E+00 1.248E-01 C1850 11 30 3.729 1.377E+00 7.662E-02 C1850 11 31 3.770 1.217E+00 6.769E-02 C1850 11 32 3.801 9.313E-01 6.017E-02 C1850 11 33 3.913 1.025E+00 4.773E-02 C1850 11 34 3.964 7.695E-01 5.655E-02 C1850 11 35 4.087 5.458E-01 4.011E-02 C1850 11 36 4.127 7.478E-01 4.831E-02 C1850 11 37 4.158 5.725E-01 3.185E-02 C1850 11 38 4.219 5.947E-01 3.309E-02 C1850 11 39 4.291 4.961E-01 3.205E-02 C1850 11 40 4.342 5.406E-01 3.973E-02 C1850 11 41 4.424 5.105E-01 3.752E-02 C1850 11 42 4.464 3.871E-01 2.154E-02 C1850 11 43 4.505 4.022E-01 2.598E-02 C1850 11 44 4.546 4.553E-01 4.143E-02 C1850 11 45 4.638 4.259E-01 3.876E-02 C1850 11 46 4.669 2.908E-01 2.137E-02 C1850 11 47 4.720 2.936E-01 1.897E-02 C1850 11 48 4.791 2.936E-01 1.897E-02 C1850 11 49 4.832 4.685E-01 C1850 11 50 4.893 1.748E+00 C1850 11 51 5.016 7.107E+00 C1850 11 52 5.057 7.314E+00 C1850 11 53 5.098 6.973E+00 C1850 11 54 5.128 3.576E+00 C1850 11 55 5.159 1.288E+00 C1850 11 56 5.200 3.726E-01 C1850 11 57 5.261 2.643E-01 C1850 11 58 5.292 1.688E-01 C1850 11 59 ENDDATA 32 0 C1850 11 60 ENDSUBENT 59 0 C1850 1199999 SUBENT C1850012 20180315 C174C1850 12 1 BIB 5 18 C1850 12 2 REACTION (6-C-12(P,X)2-HE-4,,DA/DE) C1850 12 3 SAMPLE A thin self-supported polystyrene (CH) target located C1850 12 4 at the center of a 1 m diam. scattering chamber. C1850 12 5 Targets of thicknesses ranging from 50 to C1850 12 6 150 microg/cm2 were used. C1850 12 7 DETECTOR (SIBAR) The alpha spectra were measured using a thin C1850 12 8 Ortec Surface Barrier detector (50 microm thickness, C1850 12 9 totally depleted at a reverse bias of about 100 V). C1850 12 10 ERR-ANALYS (DATA-ERR) The absolute differential cross sections C1850 12 11 for the ground state group are accurate to within C1850 12 12 about 25%. The large uncertainty is due to the fact C1850 12 13 that the usual precautions with regard to charge C1850 12 14 collection have not been carefully observed since the C1850 12 15 main emphasis in this experiment was on energy C1850 12 16 spectra. In those cases where the continuous spectra C1850 12 17 are well described by the four-body shape, the C1850 12 18 breakup cross section is accurate to within 25 %. C1850 12 19 STATUS (CURVE) Fig. 4, page 123. C1850 12 20 ENDBIB 18 0 C1850 12 21 COMMON 2 3 C1850 12 22 EN ANG C1850 12 23 MEV ADEG C1850 12 24 12.7 22.0 C1850 12 25 ENDCOMMON 3 0 C1850 12 26 DATA 3 53 C1850 12 27 E-CM DATA-CM DATA-ERR C1850 12 28 MEV MB/SR/MEV MB/SR/MEV C1850 12 29 1.105 1.031E+01 5.151E-01 C1850 12 30 1.150 1.014E+01 5.882E-01 C1850 12 31 1.182 9.385E+00 4.689E-01 C1850 12 32 1.214 9.306E+00 4.649E-01 C1850 12 33 1.241 8.917E+00 5.175E-01 C1850 12 34 1.282 8.257E+00 4.125E-01 C1850 12 35 1.309 7.452E+00 3.116E-01 C1850 12 36 1.354 7.516E+00 4.362E-01 C1850 12 37 1.395 7.141E+00 4.144E-01 C1850 12 38 1.413 6.726E+00 4.443E-01 C1850 12 39 1.449 6.726E+00 4.977E-01 C1850 12 40 1.508 6.726E+00 3.904E-01 C1850 12 41 1.535 6.669E+00 4.405E-01 C1850 12 42 1.567 6.123E+00 4.531E-01 C1850 12 43 1.608 6.123E+00 3.554E-01 C1850 12 44 1.631 6.019E+00 4.454E-01 C1850 12 45 1.676 5.918E+00 3.434E-01 C1850 12 46 1.708 6.071E+00 3.524E-01 C1850 12 47 1.758 5.867E+00 3.405E-01 C1850 12 48 1.785 5.867E+00 3.405E-01 C1850 12 49 1.808 5.622E+00 2.809E-01 C1850 12 50 1.862 6.019E+00 3.007E-01 C1850 12 51 1.898 5.768E+00 2.881E-01 C1850 12 52 1.921 5.387E+00 2.691E-01 C1850 12 53 1.957 5.206E+00 3.438E-01 C1850 12 54 1.993 5.118E+00 2.970E-01 C1850 12 55 2.039 4.862E+00 2.429E-01 C1850 12 56 2.075 4.739E+00 2.368E-01 C1850 12 57 2.098 4.464E+00 1.499E-01 C1850 12 58 2.143 3.828E+00 2.528E-01 C1850 12 59 2.188 3.426E+00 1.988E-01 C1850 12 60 2.225 2.767E+00 1.606E-01 C1850 12 61 2.261 2.476E+00 1.635E-01 C1850 12 62 2.284 1.949E+00 1.596E-01 C1850 12 63 2.324 1.672E+00 1.237E-01 C1850 12 64 2.370 1.588E+00 1.175E-01 C1850 12 65 2.415 1.362E+00 C1850 12 66 2.447 1.119E+00 C1850 12 67 2.569 7.951E-01 C1850 12 68 2.606 7.115E-01 C1850 12 69 2.633 6.206E-01 C1850 12 70 2.664 5.896E-01 C1850 12 71 2.683 5.367E-01 C1850 12 72 2.705 5.896E-01 C1850 12 73 2.755 2.105E+00 C1850 12 74 2.800 1.076E+01 C1850 12 75 2.837 3.211E+01 C1850 12 76 2.868 4.184E+01 C1850 12 77 2.927 2.730E+01 C1850 12 78 2.964 8.117E+00 C1850 12 79 2.973 1.339E+00 C1850 12 80 3.023 1.845E-01 C1850 12 81 3.068 9.318E-02 C1850 12 82 ENDDATA 55 0 C1850 12 83 ENDSUBENT 82 0 C1850 1299999 SUBENT C1850013 20180315 C174C1850 13 1 BIB 5 18 C1850 13 2 REACTION (6-C-12(P,X)2-HE-4,,DA/DE) C1850 13 3 SAMPLE A thin self-supported polystyrene (CH) target located C1850 13 4 at the center of a 1 m diam. scattering chamber. C1850 13 5 Targets of thicknesses ranging from 50 to C1850 13 6 150 microg/cm2 were used. C1850 13 7 DETECTOR (SIBAR) The alpha spectra were measured using a thin C1850 13 8 Ortec Surface Barrier detector (50 microm thickness, C1850 13 9 totally depleted at a reverse bias of about 100 V). C1850 13 10 ERR-ANALYS (DATA-ERR) The absolute differential cross sections C1850 13 11 for the ground state group are accurate to within C1850 13 12 about 25%. The large uncertainty is due to the fact C1850 13 13 that the usual precautions with regard to charge C1850 13 14 collection have not been carefully observed since the C1850 13 15 main emphasis in this experiment was on energy C1850 13 16 spectra. In those cases where the continuous spectra C1850 13 17 are well described by the four-body shape, the C1850 13 18 breakup cross section is accurate to within 25 %. C1850 13 19 STATUS (CURVE) Fig. 4, page 123. C1850 13 20 ENDBIB 18 0 C1850 13 21 COMMON 2 3 C1850 13 22 EN ANG C1850 13 23 MEV ADEG C1850 13 24 12.7 30.0 C1850 13 25 ENDCOMMON 3 0 C1850 13 26 DATA 3 51 C1850 13 27 E-CM DATA-CM DATA-ERR C1850 13 28 MEV MB/SR/MEV MB/SR/MEV C1850 13 29 1.159 7.411E+00 3.105E-01 C1850 13 30 1.182 6.518E+00 3.263E-01 C1850 13 31 1.223 6.245E+00 3.127E-01 C1850 13 32 1.259 6.462E+00 3.236E-01 C1850 13 33 1.295 6.298E+00 3.664E-01 C1850 13 34 1.318 5.635E+00 3.730E-01 C1850 13 35 1.363 5.684E+00 2.846E-01 C1850 13 36 1.390 5.173E+00 3.424E-01 C1850 13 37 1.422 5.353E+00 2.680E-01 C1850 13 38 1.454 5.217E+00 2.612E-01 C1850 13 39 1.504 5.307E+00 2.224E-01 C1850 13 40 1.535 5.262E+00 3.483E-01 C1850 13 41 1.563 5.129E+00 2.568E-01 C1850 13 42 1.599 5.173E+00 2.590E-01 C1850 13 43 1.640 5.217E+00 3.453E-01 C1850 13 44 1.676 4.999E+00 2.503E-01 C1850 13 45 1.712 5.042E+00 2.932E-01 C1850 13 46 1.753 5.042E+00 2.524E-01 C1850 13 47 1.794 5.307E+00 3.087E-01 C1850 13 48 1.826 4.668E+00 2.337E-01 C1850 13 49 1.866 4.748E+00 2.762E-01 C1850 13 50 1.912 4.285E+00 2.492E-01 C1850 13 51 1.953 4.472E+00 3.316E-01 C1850 13 52 1.980 3.833E+00 2.230E-01 C1850 13 53 2.057 3.642E+00 2.118E-01 C1850 13 54 2.089 3.258E+00 2.416E-01 C1850 13 55 2.129 2.793E+00 2.291E-01 C1850 13 56 2.170 2.520E+00 1.668E-01 C1850 13 57 2.207 2.373E+00 1.760E-01 C1850 13 58 2.234 2.142E+00 1.418E-01 C1850 13 59 2.275 1.685E+00 1.116E-01 C1850 13 60 2.311 1.587E+00 9.232E-02 C1850 13 61 2.356 1.292E+00 8.555E-02 C1850 13 62 2.406 1.217E+00 8.058E-02 C1850 13 63 2.451 1.052E+00 8.635E-02 C1850 13 64 2.479 9.256E-01 7.594E-02 C1850 13 65 2.528 7.866E-01 6.454E-02 C1850 13 66 2.565 7.038E-01 6.871E-02 C1850 13 67 2.601 6.033E-01 4.474E-02 C1850 13 68 2.615 5.491E-01 3.194E-02 C1850 13 69 2.674 5.127E-01 2.567E-02 C1850 13 70 2.696 4.666E-01 3.089E-02 C1850 13 71 2.755 7.409E-01 C1850 13 72 2.787 4.212E+00 C1850 13 73 2.805 1.686E+01 C1850 13 74 2.850 3.149E+01 C1850 13 75 2.900 3.017E+01 C1850 13 76 2.923 1.521E+01 C1850 13 77 2.955 4.141E+00 C1850 13 78 2.991 6.460E-01 C1850 13 79 3.023 9.741E-02 C1850 13 80 ENDDATA 53 0 C1850 13 81 ENDSUBENT 80 0 C1850 1399999 SUBENT C1850014 20180315 C174C1850 14 1 BIB 5 18 C1850 14 2 REACTION (6-C-12(P,X)2-HE-4,,DA/DE) C1850 14 3 SAMPLE A thin self-supported polystyrene (CH) target located C1850 14 4 at the center of a 1 m diam. scattering chamber. C1850 14 5 Targets of thicknesses ranging from 50 to C1850 14 6 150 microg/cm2 were used. C1850 14 7 DETECTOR (SIBAR) The alpha spectra were measured using a thin C1850 14 8 Ortec Surface Barrier detector (50 microm thickness, C1850 14 9 totally depleted at a reverse bias of about 100 V). C1850 14 10 ERR-ANALYS (DATA-ERR) The absolute differential cross sections C1850 14 11 for the ground state group are accurate to within C1850 14 12 about 25%. The large uncertainty is due to the fact C1850 14 13 that the usual precautions with regard to charge C1850 14 14 collection have not been carefully observed since the C1850 14 15 main emphasis in this experiment was on energy C1850 14 16 spectra. In those cases where the continuous spectra C1850 14 17 are well described by the four-body shape, the C1850 14 18 breakup cross section is accurate to within 25 %. C1850 14 19 STATUS (CURVE) Fig. 4, page 123. C1850 14 20 ENDBIB 18 0 C1850 14 21 COMMON 2 3 C1850 14 22 EN ANG C1850 14 23 MEV ADEG C1850 14 24 12.7 45.0 C1850 14 25 ENDCOMMON 3 0 C1850 14 26 DATA 3 41 C1850 14 27 E-CM DATA-CM DATA-ERR C1850 14 28 MEV MB/SR/MEV MB/SR/MEV C1850 14 29 1.413 7.273E+00 3.660E-01 C1850 14 30 1.427 5.865E+00 2.952E-01 C1850 14 31 1.467 5.428E+00 3.611E-01 C1850 14 32 1.508 5.110E+00 4.214E-01 C1850 14 33 1.545 5.289E+00 3.093E-01 C1850 14 34 1.585 5.428E+00 3.173E-01 C1850 14 35 1.622 4.937E+00 3.680E-01 C1850 14 36 1.658 5.199E+00 3.040E-01 C1850 14 37 1.699 4.980E+00 4.107E-01 C1850 14 38 1.726 4.649E+00 3.834E-01 C1850 14 39 1.771 4.491E+00 3.348E-01 C1850 14 40 1.798 4.812E+00 3.201E-01 C1850 14 41 1.862 4.609E+00 3.435E-01 C1850 14 42 1.894 4.339E+00 3.234E-01 C1850 14 43 1.916 4.051E+00 2.368E-01 C1850 14 44 1.962 4.051E+00 2.695E-01 C1850 14 45 2.012 3.685E+00 2.746E-01 C1850 14 46 2.057 3.469E+00 2.586E-01 C1850 14 47 2.089 2.774E+00 2.067E-01 C1850 14 48 2.111 2.921E+00 1.943E-01 C1850 14 49 2.152 2.438E+00 1.622E-01 C1850 14 50 2.202 2.143E+00 1.597E-01 C1850 14 51 2.247 2.052E+00 1.692E-01 C1850 14 52 2.284 1.899E+00 1.566E-01 C1850 14 53 2.315 1.655E+00 1.495E-01 C1850 14 54 2.374 1.417E+00 1.169E-01 C1850 14 55 2.401 1.246E+00 8.289E-02 C1850 14 56 2.447 1.204E+00 8.009E-02 C1850 14 57 2.483 1.204E+00 8.009E-02 C1850 14 58 2.519 9.060E-01 6.753E-02 C1850 14 59 2.560 7.059E-01 4.697E-02 C1850 14 60 2.606 7.306E-01 4.861E-02 C1850 14 61 2.633 5.547E-01 4.575E-02 C1850 14 62 2.696 5.178E-01 3.860E-02 C1850 14 63 2.732 5.841E-01 C1850 14 64 2.746 1.031E+00 C1850 14 65 2.805 4.121E+00 C1850 14 66 2.868 1.460E+01 C1850 14 67 2.914 1.229E+01 C1850 14 68 2.950 3.847E+00 C1850 14 69 2.991 5.841E-01 C1850 14 70 ENDDATA 43 0 C1850 14 71 ENDSUBENT 70 0 C1850 1499999 SUBENT C1850015 20180315 C174C1850 15 1 BIB 5 18 C1850 15 2 REACTION (6-C-12(P,A)5-B-9,,DA/DE) C1850 15 3 SAMPLE A thin self-supported polystyrene (CH) target located C1850 15 4 at the center of a 1 m diam. scattering chamber. C1850 15 5 Targets of thicknesses ranging from 50 to C1850 15 6 150 microg/cm2 were used. C1850 15 7 DETECTOR (SIBAR) The alpha spectra were measured using a thin C1850 15 8 Ortec Surface Barrier detector (50 microm thickness, C1850 15 9 totally depleted at a reverse bias of about 100 V). C1850 15 10 ERR-ANALYS (DATA-ERR) The absolute differential cross sections C1850 15 11 for the ground state group are accurate to within C1850 15 12 about 25%. The large uncertainty is due to the fact C1850 15 13 that the usual precautions with regard to charge C1850 15 14 collection have not been carefully observed since the C1850 15 15 main emphasis in this experiment was on energy C1850 15 16 spectra. In those cases where the continuous spectra C1850 15 17 are well described by the four-body shape, the C1850 15 18 breakup cross section is accurate to within 25 %. C1850 15 19 STATUS (CURVE) Fig. 4, page 123. C1850 15 20 ENDBIB 18 0 C1850 15 21 COMMON 2 3 C1850 15 22 EN ANG C1850 15 23 MEV ADEG C1850 15 24 12.7 60.0 C1850 15 25 ENDCOMMON 3 0 C1850 15 26 DATA 3 30 C1850 15 27 E-CM DATA-CM DATA-ERR C1850 15 28 MEV MB/SR/MEV MB/SR/MEV C1850 15 29 1.784 3.106E+00 2.285E-01 C1850 15 30 1.829 2.902E+00 1.676E-01 C1850 15 31 1.884 2.429E+00 1.789E-01 C1850 15 32 1.911 2.328E+00 1.345E-01 C1850 15 33 1.957 2.289E+00 1.324E-01 C1850 15 34 1.984 2.213E+00 1.101E-01 C1850 15 35 2.043 1.999E+00 1.154E-01 C1850 15 36 2.084 1.950E+00 1.589E-01 C1850 15 37 2.121 1.485E+00 4.963E-02 C1850 15 38 2.162 1.564E+00 1.028E-01 C1850 15 39 2.207 1.331E+00 9.794E-02 C1850 15 40 2.248 1.233E+00 9.089E-02 C1850 15 41 2.298 1.223E+00 9.008E-02 C1850 15 42 2.353 1.023E+00 7.541E-02 C1850 15 43 2.389 9.088E-01 3.783E-02 C1850 15 44 2.430 8.565E-01 4.947E-02 C1850 15 45 2.462 8.281E-01 6.096E-02 C1850 15 46 2.508 6.364E-01 5.186E-02 C1850 15 47 2.540 6.642E-01 3.834E-02 C1850 15 48 2.604 5.372E-01 2.671E-02 C1850 15 49 2.640 4.381E-01 5.573E-02 C1850 15 50 2.677 3.957E-01 1.967E-02 C1850 15 51 2.739 7.429E-01 C1850 15 52 2.773 2.465E+00 C1850 15 53 2.803 6.391E+00 C1850 15 54 2.842 1.029E+01 C1850 15 55 2.883 1.004E+01 C1850 15 56 2.925 6.026E+00 C1850 15 57 2.959 2.642E+00 C1850 15 58 3.006 7.635E-01 C1850 15 59 ENDDATA 32 0 C1850 15 60 ENDSUBENT 59 0 C1850 1599999 SUBENT C1850016 20180315 C174C1850 16 1 BIB 7 24 C1850 16 2 REACTION (4-BE-9(P,X)0-NN-1,,DA/DE) C1850 16 3 SAMPLE A 1.28 mg/cm2 Be target evaporated on a 0.5 mm thick C1850 16 4 tantalum plate which was thick enough to stop the C1850 16 5 proton beam. C1850 16 6 DETECTOR (SCIN) The neutron detectors, consisting of 5 x 5 cm C1850 16 7 plastic scintillators mounted on RCA-6655 C1850 16 8 photomultipliers, were positioned, at 15 degree C1850 16 9 angular intervals in a well collimated and shielded C1850 16 10 geometry. C1850 16 11 METHOD (TOF) The neutron spectra were observed using time-of- C1850 16 12 flight techniques. A flight-path of about 10 m was C1850 16 13 chosen as an optimum considering neutron intensities C1850 16 14 and resolution of the experimental equipment. C1850 16 15 REL-REF (M,,J.D.Anderson+,J,NIM,15,178,1962) C1850 16 16 ERR-ANALYS (DATA-ERR) The absolute differential cross sections C1850 16 17 for the ground state group are accurate to within C1850 16 18 about 25%. The large uncertainty is due to the fact C1850 16 19 that the usual precautions with regard to charge C1850 16 20 collection have not been carefully observed since the C1850 16 21 main emphasis in this experiment was on energy C1850 16 22 spectra. In those cases where the continuous spectra C1850 16 23 are well described by the four-body shape, the C1850 16 24 breakup cross section is accurate to within 25 %. C1850 16 25 STATUS (CURVE) Fig. 5, page 125. C1850 16 26 ENDBIB 24 0 C1850 16 27 COMMON 2 3 C1850 16 28 EN ANG C1850 16 29 MEV ADEG C1850 16 30 7.4 15.0 C1850 16 31 ENDCOMMON 3 0 C1850 16 32 DATA 3 94 C1850 16 33 E-CM DATA-CM DATA-ERR C1850 16 34 MEV MB/SR/MEV MB/SR/MEV C1850 16 35 0.100 1.545E+00 C1850 16 36 0.162 1.774E+00 C1850 16 37 0.189 2.037E+00 C1850 16 38 0.268 1.997E+00 C1850 16 39 0.313 1.882E+00 C1850 16 40 0.340 1.576E+00 C1850 16 41 0.411 1.774E+00 C1850 16 42 0.482 1.845E+00 C1850 16 43 0.526 1.997E+00 C1850 16 44 0.588 2.119E+00 C1850 16 45 0.677 2.037E+00 2.278E-01 C1850 16 46 0.775 1.774E+00 C1850 16 47 0.846 1.705E+00 C1850 16 48 0.873 1.456E+00 C1850 16 49 0.917 1.345E+00 C1850 16 50 0.944 1.219E+00 C1850 16 51 0.980 1.040E+00 C1850 16 52 1.042 1.020E+00 C1850 16 53 1.086 1.171E+00 C1850 16 54 1.104 6.474E-01 2.524E-01 C1850 16 55 1.157 9.804E-01 C1850 16 56 1.184 1.148E+00 C1850 16 57 1.228 1.268E+00 C1850 16 58 1.264 1.427E+00 C1850 16 59 1.299 1.920E+00 C1850 16 60 1.388 4.581E+00 C1850 16 61 1.424 8.794E+00 C1850 16 62 1.477 1.137E+01 1.272E+00 C1850 16 63 1.531 1.010E+01 C1850 16 64 1.628 2.907E+00 C1850 16 65 1.682 1.082E+00 C1850 16 66 1.753 4.536E-01 C1850 16 67 1.779 2.660E-01 C1850 16 68 1.842 2.227E-01 4.351E-02 C1850 16 69 1.957 2.017E-01 C1850 16 70 1.993 2.227E-01 C1850 16 71 2.073 2.057E-01 C1850 16 72 2.126 1.500E-01 C1850 16 73 2.179 1.623E-01 C1850 16 74 2.215 1.864E-01 C1850 16 75 2.268 1.530E-01 C1850 16 76 2.304 1.623E-01 C1850 16 77 2.366 1.591E-01 C1850 16 78 2.455 1.386E-01 C1850 16 79 2.562 1.207E-01 1.559E-02 C1850 16 80 2.579 8.970E-02 C1850 16 81 2.624 1.137E-01 C1850 16 82 2.650 8.970E-02 C1850 16 83 2.659 7.076E-02 C1850 16 84 2.722 6.802E-02 C1850 16 85 2.722 8.622E-02 C1850 16 86 2.775 1.051E-01 C1850 16 87 2.810 7.361E-02 C1850 16 88 2.873 6.285E-02 C1850 16 89 2.899 5.057E-02 C1850 16 90 2.926 6.938E-02 C1850 16 91 2.970 4.317E-02 C1850 16 92 2.988 5.693E-02 C1850 16 93 3.024 6.938E-02 C1850 16 94 3.059 4.317E-02 C1850 16 95 3.148 6.938E-02 C1850 16 96 3.166 3.474E-02 5.661E-03 C1850 16 97 3.219 2.740E-02 C1850 16 98 3.237 3.339E-02 C1850 16 99 3.299 3.989E-02 C1850 16 100 3.326 5.693E-02 C1850 16 101 3.353 3.543E-02 C1850 16 102 3.379 3.147E-02 C1850 16 103 3.406 2.294E-02 C1850 16 104 3.450 1.639E-02 C1850 16 105 3.468 4.233E-02 C1850 16 106 3.557 2.795E-02 C1850 16 107 3.566 1.882E-02 C1850 16 108 3.601 3.274E-02 C1850 16 109 3.619 5.261E-02 C1850 16 110 3.681 3.989E-02 C1850 16 111 3.726 7.217E-02 C1850 16 112 3.744 1.280E-01 2.296E-02 C1850 16 113 3.770 2.057E-01 C1850 16 114 3.832 3.722E-01 C1850 16 115 3.841 5.637E-01 C1850 16 116 3.912 8.046E-01 C1850 16 117 3.939 1.809E+00 C1850 16 118 4.019 2.851E+00 C1850 16 119 4.099 3.209E+00 3.589E-01 C1850 16 120 4.161 3.085E+00 C1850 16 121 4.232 2.294E+00 C1850 16 122 4.277 2.037E+00 C1850 16 123 4.312 1.195E+00 C1850 16 124 4.463 1.978E-01 C1850 16 125 4.508 6.041E-02 C1850 16 126 4.570 1.485E-02 C1850 16 127 4.606 3.440E-03 C1850 16 128 4.650 8.126E-04 C1850 16 129 ENDDATA 96 0 C1850 16 130 ENDSUBENT 129 0 C1850 1699999 SUBENT C1850017 20180315 C174C1850 17 1 BIB 7 24 C1850 17 2 REACTION (4-BE-9(P,X)0-NN-1,,DA/DE) C1850 17 3 SAMPLE A 1.28 mg/cm2 Be target evaporated on a 0.5 mm thick C1850 17 4 tantalum plate which was thick enough to stop the C1850 17 5 proton beam. C1850 17 6 DETECTOR (SCIN) The neutron detectors, consisting of 5 x 5 cm C1850 17 7 plastic scintillators mounted on RCA-6655 C1850 17 8 photomultipliers, were positioned, at 15 degree C1850 17 9 angular intervals in a well collimated and shielded C1850 17 10 geometry. C1850 17 11 METHOD (TOF) The neutron spectra were observed using time-of- C1850 17 12 flight techniques. A flight-path of about 10 m was C1850 17 13 chosen as an optimum considering neutron intensities C1850 17 14 and resolution of the experimental equipment. C1850 17 15 REL-REF (M,,J.D.Anderson+,J,NIM,15,178,1962) C1850 17 16 ERR-ANALYS (DATA-ERR) The absolute differential cross sections C1850 17 17 for the ground state group are accurate to within C1850 17 18 about 25%. The large uncertainty is due to the fact C1850 17 19 that the usual precautions with regard to charge C1850 17 20 collection have not been carefully observed since the C1850 17 21 main emphasis in this experiment was on energy C1850 17 22 spectra. In those cases where the continuous spectra C1850 17 23 are well described by the four-body shape, the C1850 17 24 breakup cross section is accurate to within 25 %. C1850 17 25 STATUS (CURVE) Fig. 5, page 125. C1850 17 26 ENDBIB 24 0 C1850 17 27 COMMON 2 3 C1850 17 28 EN ANG C1850 17 29 MEV ADEG C1850 17 30 7.4 45.0 C1850 17 31 ENDCOMMON 3 0 C1850 17 32 DATA 3 69 C1850 17 33 E-CM DATA-CM DATA-ERR C1850 17 34 MEV MB/SR/MEV MB/SR/MEV C1850 17 35 0.473 1.174E+01 C1850 17 36 0.517 1.068E+01 C1850 17 37 0.580 1.058E+01 C1850 17 38 0.677 9.099E+00 4.198E-01 C1850 17 39 0.748 9.449E+00 C1850 17 40 0.793 8.761E+00 C1850 17 41 0.864 8.597E+00 C1850 17 42 0.900 8.928E+00 C1850 17 43 1.006 9.013E+00 C1850 17 44 1.086 8.436E+00 C1850 17 45 1.113 9.360E+00 C1850 17 46 1.211 9.360E+00 C1850 17 47 1.291 1.109E+01 C1850 17 48 1.379 1.392E+01 C1850 17 49 1.415 1.730E+01 C1850 17 50 1.451 2.253E+01 C1850 17 51 1.531 2.524E+01 1.391E+00 C1850 17 52 1.584 1.848E+01 C1850 17 53 1.628 1.099E+01 C1850 17 54 1.691 7.050E+00 C1850 17 55 1.726 5.620E+00 C1850 17 56 1.779 4.697E+00 C1850 17 57 1.842 4.653E+00 C1850 17 58 1.957 4.038E+00 2.939E-01 C1850 17 59 2.019 3.815E+00 C1850 17 60 2.090 4.273E+00 C1850 17 61 2.126 3.744E+00 C1850 17 62 2.250 3.504E+00 C1850 17 63 2.313 3.407E+00 C1850 17 64 2.348 3.249E+00 C1850 17 65 2.384 2.874E+00 C1850 17 66 2.464 3.311E+00 C1850 17 67 2.570 3.129E+00 C1850 17 68 2.633 2.957E+00 C1850 17 69 2.704 2.901E+00 C1850 17 70 2.775 2.045E+00 C1850 17 71 2.935 2.313E+00 C1850 17 72 2.953 1.585E+00 C1850 17 73 3.041 2.379E+00 C1850 17 74 3.041 2.185E+00 C1850 17 75 3.077 1.541E+00 C1850 17 76 3.175 1.470E+00 3.415E-01 C1850 17 77 3.219 2.227E+00 C1850 17 78 3.246 1.759E+00 C1850 17 79 3.255 1.631E+00 C1850 17 80 3.308 1.600E+00 C1850 17 81 3.344 1.933E+00 C1850 17 82 3.344 1.709E+00 C1850 17 83 3.406 2.448E+00 C1850 17 84 3.406 1.662E+00 C1850 17 85 3.495 2.379E+00 C1850 17 86 3.601 2.165E+00 C1850 17 87 3.690 3.571E+00 C1850 17 88 3.850 7.532E+00 C1850 17 89 3.859 9.185E+00 C1850 17 90 3.921 1.120E+01 C1850 17 91 3.975 1.634E+01 1.046E+00 C1850 17 92 4.001 1.901E+01 C1850 17 93 4.144 2.211E+01 C1850 17 94 4.250 1.619E+01 C1850 17 95 4.304 1.163E+01 C1850 17 96 4.321 7.676E+00 C1850 17 97 4.375 4.971E+00 C1850 17 98 4.410 3.639E+00 C1850 17 99 4.455 2.402E+00 C1850 17 100 4.499 1.171E+00 C1850 17 101 4.543 6.400E-01 C1850 17 102 4.570 4.428E-01 C1850 17 103 4.659 2.840E-01 C1850 17 104 ENDDATA 71 0 C1850 17 105 ENDSUBENT 104 0 C1850 1799999 SUBENT C1850018 20180315 C174C1850 18 1 BIB 7 24 C1850 18 2 REACTION (4-BE-9(P,X)0-NN-1,,DA/DE) C1850 18 3 SAMPLE A 1.28 mg/cm2 Be target evaporated on a 0.5 mm thick C1850 18 4 tantalum plate which was thick enough to stop the C1850 18 5 proton beam. C1850 18 6 DETECTOR (SCIN) The neutron detectors, consisting of 5 x 5 cm C1850 18 7 plastic scintillators mounted on RCA-6655 C1850 18 8 photomultipliers, were positioned, at 15 degree C1850 18 9 angular intervals in a well collimated and shielded C1850 18 10 geometry. C1850 18 11 METHOD (TOF) The neutron spectra were observed using time-of- C1850 18 12 flight techniques. A flight-path of about 10 m was C1850 18 13 chosen as an optimum considering neutron intensities C1850 18 14 and resolution of the experimental equipment. C1850 18 15 REL-REF (M,,J.D.Anderson+,J,NIM,15,178,1962) C1850 18 16 ERR-ANALYS (DATA-ERR) The absolute differential cross sections C1850 18 17 for the ground state group are accurate to within C1850 18 18 about 25%. The large uncertainty is due to the fact C1850 18 19 that the usual precautions with regard to charge C1850 18 20 collection have not been carefully observed since the C1850 18 21 main emphasis in this experiment was on energy C1850 18 22 spectra. In those cases where the continuous spectra C1850 18 23 are well described by the four-body shape, the C1850 18 24 breakup cross section is accurate to within 25 %. C1850 18 25 STATUS (CURVE) Fig. 5, page 125. C1850 18 26 ENDBIB 24 0 C1850 18 27 COMMON 2 3 C1850 18 28 EN ANG C1850 18 29 MEV ADEG C1850 18 30 7.4 75.0 C1850 18 31 ENDCOMMON 3 0 C1850 18 32 DATA 3 64 C1850 18 33 E-CM DATA-CM DATA-ERR C1850 18 34 MEV MB/SR/MEV MB/SR/MEV C1850 18 35 0.864 8.051E+00 6.831E-01 C1850 18 36 0.997 7.816E+00 C1850 18 37 1.059 7.296E+00 C1850 18 38 1.104 7.664E+00 C1850 18 39 1.166 7.368E+00 C1850 18 40 1.246 7.664E+00 C1850 18 41 1.291 8.131E+00 C1850 18 42 1.371 8.051E+00 C1850 18 43 1.433 1.384E+01 C1850 18 44 1.504 2.356E+01 C1850 18 45 1.539 2.956E+01 C1850 18 46 1.593 1.824E+01 C1850 18 47 1.655 8.972E+00 C1850 18 48 1.726 5.703E+00 C1850 18 49 1.771 3.661E+00 C1850 18 50 1.851 3.733E+00 C1850 18 51 1.957 3.383E+00 4.934E-01 C1850 18 52 2.010 2.542E+00 C1850 18 53 2.055 2.697E+00 C1850 18 54 2.144 2.619E+00 C1850 18 55 2.259 2.193E+00 C1850 18 56 2.313 1.783E+00 C1850 18 57 2.384 1.783E+00 C1850 18 58 2.437 1.731E+00 C1850 18 59 2.499 1.422E+00 C1850 18 60 2.553 1.340E+00 C1850 18 61 2.730 1.133E+00 C1850 18 62 2.855 9.126E-01 C1850 18 63 2.890 9.972E-01 C1850 18 64 2.961 9.307E-01 C1850 18 65 3.041 7.347E-01 C1850 18 66 3.086 8.517E-01 C1850 18 67 3.193 8.517E-01 C1850 18 68 3.290 8.351E-01 C1850 18 69 3.344 5.916E-01 C1850 18 70 3.406 7.063E-01 C1850 18 71 3.539 2.560E-01 C1850 18 72 3.575 5.858E-01 C1850 18 73 3.584 7.718E-01 C1850 18 74 3.619 4.858E-01 C1850 18 75 3.637 3.650E-01 C1850 18 76 3.681 8.108E-01 C1850 18 77 3.690 6.338E-01 C1850 18 78 3.779 1.027E+00 2.001E-01 C1850 18 79 3.815 7.718E-01 C1850 18 80 3.895 1.464E+00 C1850 18 81 3.930 2.150E+00 C1850 18 82 3.948 3.252E+00 C1850 18 83 3.984 4.637E+00 C1850 18 84 4.046 9.426E+00 C1850 18 85 4.072 1.589E+01 C1850 18 86 4.081 2.033E+01 C1850 18 87 4.135 2.310E+01 C1850 18 88 4.152 2.841E+01 1.631E+00 C1850 18 89 4.241 2.813E+01 C1850 18 90 4.295 1.702E+01 C1850 18 91 4.321 1.230E+01 C1850 18 92 4.357 6.050E+00 C1850 18 93 4.455 2.976E+00 C1850 18 94 4.508 8.517E-01 C1850 18 95 4.552 9.972E-01 C1850 18 96 4.579 7.420E-01 C1850 18 97 4.650 8.188E-01 C1850 18 98 4.677 5.743E-01 C1850 18 99 ENDDATA 66 0 C1850 18 100 ENDSUBENT 99 0 C1850 1899999 SUBENT C1850019 20180315 C174C1850 19 1 BIB 7 24 C1850 19 2 REACTION (4-BE-9(P,X)0-NN-1,,DA/DE) C1850 19 3 SAMPLE A 1.28 mg/cm2 Be target evaporated on a 0.5 mm thick C1850 19 4 tantalum plate which was thick enough to stop the C1850 19 5 proton beam. C1850 19 6 DETECTOR (SCIN) The neutron detectors, consisting of 5 x 5 cm C1850 19 7 plastic scintillators mounted on RCA-6655 C1850 19 8 photomultipliers, were positioned, at 15 degree C1850 19 9 angular intervals in a well collimated and shielded C1850 19 10 geometry. C1850 19 11 METHOD (TOF) The neutron spectra were observed using time-of- C1850 19 12 flight techniques. A flight-path of about 10 m was C1850 19 13 chosen as an optimum considering neutron intensities C1850 19 14 and resolution of the experimental equipment. C1850 19 15 REL-REF (M,,J.D.Anderson+,J,NIM,15,178,1962) C1850 19 16 ERR-ANALYS (DATA-ERR) The absolute differential cross sections C1850 19 17 for the ground state group are accurate to within C1850 19 18 about 25%. The large uncertainty is due to the fact C1850 19 19 that the usual precautions with regard to charge C1850 19 20 collection have not been carefully observed since the C1850 19 21 main emphasis in this experiment was on energy C1850 19 22 spectra. In those cases where the continuous spectra C1850 19 23 are well described by the four-body shape, the C1850 19 24 breakup cross section is accurate to within 25 %. C1850 19 25 STATUS (CURVE) Fig. 5, page 125. C1850 19 26 ENDBIB 24 0 C1850 19 27 COMMON 2 3 C1850 19 28 EN ANG C1850 19 29 MEV ADEG C1850 19 30 7.4 105.0 C1850 19 31 ENDCOMMON 3 0 C1850 19 32 DATA 3 50 C1850 19 33 E-CM DATA-CM DATA-ERR C1850 19 34 MEV MB/SR/MEV MB/SR/MEV C1850 19 35 1.228 8.241E+00 C1850 19 36 1.299 7.845E+00 6.655E-01 C1850 19 37 1.362 8.323E+00 C1850 19 38 1.424 1.129E+01 C1850 19 39 1.504 1.904E+01 C1850 19 40 1.575 2.966E+01 C1850 19 41 1.655 2.687E+01 C1850 19 42 1.717 1.389E+01 C1850 19 43 1.771 6.971E+00 C1850 19 44 1.833 3.748E+00 C1850 19 45 1.966 3.785E+00 3.886E-01 C1850 19 46 2.028 2.603E+00 C1850 19 47 2.090 2.988E+00 C1850 19 48 2.162 2.708E+00 C1850 19 49 2.233 3.201E+00 C1850 19 50 2.304 1.844E+00 C1850 19 51 2.348 2.055E+00 C1850 19 52 2.419 1.956E+00 C1850 19 53 2.473 2.382E+00 C1850 19 54 2.588 1.544E+00 2.509E-01 C1850 19 55 2.713 1.485E+00 C1850 19 56 2.757 1.976E+00 C1850 19 57 2.810 8.553E-01 C1850 19 58 2.828 1.281E+00 C1850 19 59 2.935 1.083E+00 C1850 19 60 2.997 9.531E-01 C1850 19 61 3.077 1.021E+00 C1850 19 62 3.130 1.293E+00 C1850 19 63 3.193 1.052E+00 1.881E-01 C1850 19 64 3.299 7.983E-01 C1850 19 65 3.379 1.073E+00 C1850 19 66 3.530 1.219E+00 C1850 19 67 3.592 7.163E-01 C1850 19 68 3.655 8.553E-01 C1850 19 69 3.708 8.637E-01 2.273E-01 C1850 19 70 3.779 1.073E+00 C1850 19 71 3.859 1.544E+00 C1850 19 72 3.904 2.159E+00 C1850 19 73 3.975 3.233E+00 C1850 19 74 4.055 7.040E+00 C1850 19 75 4.117 1.309E+01 C1850 19 76 4.232 1.445E+01 1.226E+00 C1850 19 77 4.330 1.118E+01 C1850 19 78 4.384 8.743E+00 C1850 19 79 4.437 3.937E+00 C1850 19 80 4.446 2.930E+00 C1850 19 81 4.508 1.862E+00 C1850 19 82 4.526 8.984E-01 C1850 19 83 4.543 4.509E-01 C1850 19 84 4.588 4.208E-01 C1850 19 85 ENDDATA 52 0 C1850 19 86 ENDSUBENT 85 0 C1850 1999999 SUBENT C1850020 20180315 C174C1850 20 1 BIB 7 24 C1850 20 2 REACTION (4-BE-9(P,X)0-NN-1,,DA/DE) C1850 20 3 SAMPLE A 1.28 mg/cm2 Be target evaporated on a 0.5 mm thick C1850 20 4 tantalum plate which was thick enough to stop the C1850 20 5 proton beam. C1850 20 6 DETECTOR (SCIN) The neutron detectors, consisting of 5 x 5 cm C1850 20 7 plastic scintillators mounted on RCA-6655 C1850 20 8 photomultipliers, were positioned, at 15 degree C1850 20 9 angular intervals in a well collimated and shielded C1850 20 10 geometry. C1850 20 11 METHOD (TOF) The neutron spectra were observed using time-of- C1850 20 12 flight techniques. A flight-path of about 10 m was C1850 20 13 chosen as an optimum considering neutron intensities C1850 20 14 and resolution of the experimental equipment. C1850 20 15 REL-REF (M,,J.D.Anderson+,J,NIM,15,178,1962) C1850 20 16 ERR-ANALYS (DATA-ERR) The absolute differential cross sections C1850 20 17 for the ground state group are accurate to within C1850 20 18 about 25%. The large uncertainty is due to the fact C1850 20 19 that the usual precautions with regard to charge C1850 20 20 collection have not been carefully observed since the C1850 20 21 main emphasis in this experiment was on energy C1850 20 22 spectra. In those cases where the continuous spectra C1850 20 23 are well described by the four-body shape, the C1850 20 24 breakup cross section is accurate to within 25 %. C1850 20 25 STATUS (CURVE) Fig. 6, page 125. C1850 20 26 ENDBIB 24 0 C1850 20 27 COMMON 2 3 C1850 20 28 EN ANG C1850 20 29 MEV ADEG C1850 20 30 6.3 3.0 C1850 20 31 ENDCOMMON 3 0 C1850 20 32 DATA 3 85 C1850 20 33 E-CM DATA-CM DATA-ERR C1850 20 34 MEV MB/SR/MEV MB/SR/MEV C1850 20 35 0.818 1.073E+01 8.390E-01 C1850 20 36 0.870 1.184E+01 C1850 20 37 0.898 1.371E+01 C1850 20 38 0.941 1.317E+01 C1850 20 39 1.031 1.129E+01 C1850 20 40 1.059 1.383E+01 C1850 20 41 1.097 1.477E+01 C1850 20 42 1.101 1.538E+01 C1850 20 43 1.149 1.590E+01 C1850 20 44 1.191 2.063E+01 C1850 20 45 1.232 3.025E+01 C1850 20 46 1.303 4.400E+01 3.107E+00 C1850 20 47 1.346 3.448E+01 C1850 20 48 1.394 2.296E+01 C1850 20 49 1.433 1.456E+01 C1850 20 50 1.477 9.465E+00 C1850 20 51 1.558 6.203E+00 C1850 20 52 1.610 6.105E+00 C1850 20 53 1.692 3.905E+00 C1850 20 54 1.730 3.906E+00 C1850 20 55 1.768 3.486E+00 C1850 20 56 1.815 3.662E+00 C1850 20 57 1.858 2.965E+00 C1850 20 58 1.901 2.824E+00 C1850 20 59 1.949 1.836E+00 C1850 20 60 2.035 1.852E+00 3.772E-01 C1850 20 61 2.071 3.327E+00 C1850 20 62 2.104 3.383E+00 C1850 20 63 2.190 2.347E+00 C1850 20 64 2.214 2.027E+00 C1850 20 65 2.228 2.740E+00 C1850 20 66 2.247 2.348E+00 C1850 20 67 2.280 2.506E+00 C1850 20 68 2.289 3.122E+00 C1850 20 69 2.314 1.855E+00 C1850 20 70 2.329 1.539E+00 C1850 20 71 2.352 1.669E+00 C1850 20 72 2.366 2.350E+00 C1850 20 73 2.384 2.591E+00 C1850 20 74 2.400 1.725E+00 C1850 20 75 2.418 1.841E+00 C1850 20 76 2.419 1.419E+00 C1850 20 77 2.452 1.341E+00 C1850 20 78 2.477 1.042E+00 C1850 20 79 2.489 1.950E+00 C1850 20 80 2.524 1.237E+00 4.527E-01 C1850 20 81 2.594 1.984E+00 C1850 20 82 2.594 1.700E+00 C1850 20 83 2.631 2.067E+00 C1850 20 84 2.641 1.714E+00 C1850 20 85 2.672 7.062E-01 C1850 20 86 2.689 1.555E+00 C1850 20 87 2.708 1.249E+00 C1850 20 88 2.746 1.446E+00 C1850 20 89 2.756 1.209E+00 C1850 20 90 2.769 1.831E+00 C1850 20 91 2.793 1.389E+00 C1850 20 92 2.819 6.412E-01 C1850 20 93 2.837 9.173E-01 C1850 20 94 2.870 8.738E-01 C1850 20 95 2.892 1.570E+00 C1850 20 96 2.907 1.424E+00 C1850 20 97 2.936 1.324E+00 C1850 20 98 2.945 1.379E+00 C1850 20 99 2.983 1.144E+00 4.587E-01 C1850 20 100 3.041 7.314E-01 C1850 20 101 3.078 1.064E+00 C1850 20 102 3.113 6.169E-01 C1850 20 103 3.125 1.598E+00 C1850 20 104 3.190 2.461E+00 C1850 20 105 3.213 3.667E+00 C1850 20 106 3.258 7.385E+00 C1850 20 107 3.286 1.031E+01 C1850 20 108 3.337 1.736E+01 C1850 20 109 3.360 2.199E+01 C1850 20 110 3.379 2.405E+01 C1850 20 111 3.445 2.785E+01 2.998E+00 C1850 20 112 3.507 2.165E+01 C1850 20 113 3.540 1.871E+01 C1850 20 114 3.579 1.319E+01 C1850 20 115 3.594 1.033E+01 C1850 20 116 3.628 7.838E+00 C1850 20 117 3.657 4.545E+00 C1850 20 118 3.687 2.978E+00 C1850 20 119 3.712 1.386E+00 C1850 20 120 ENDDATA 87 0 C1850 20 121 ENDSUBENT 120 0 C1850 2099999 SUBENT C1850021 20180315 C174C1850 21 1 BIB 7 24 C1850 21 2 REACTION (4-BE-9(P,X)0-NN-1,,DA/DE) C1850 21 3 SAMPLE A 1.28 mg/cm2 Be target evaporated on a 0.5 mm thick C1850 21 4 tantalum plate which was thick enough to stop the C1850 21 5 proton beam. C1850 21 6 DETECTOR (SCIN) The neutron detectors, consisting of 5 x 5 cm C1850 21 7 plastic scintillators mounted on RCA-6655 C1850 21 8 photomultipliers, were positioned, at 15 degree C1850 21 9 angular intervals in a well collimated and shielded C1850 21 10 geometry. C1850 21 11 METHOD (TOF) The neutron spectra were observed using time-of- C1850 21 12 flight techniques. A flight-path of about 10 m was C1850 21 13 chosen as an optimum considering neutron intensities C1850 21 14 and resolution of the experimental equipment. C1850 21 15 REL-REF (M,,J.D.Anderson+,J,NIM,15,178,1962) C1850 21 16 ERR-ANALYS (DATA-ERR) The absolute differential cross sections C1850 21 17 for the ground state group are accurate to within C1850 21 18 about 25%. The large uncertainty is due to the fact C1850 21 19 that the usual precautions with regard to charge C1850 21 20 collection have not been carefully observed since the C1850 21 21 main emphasis in this experiment was on energy C1850 21 22 spectra. In those cases where the continuous spectra C1850 21 23 are well described by the four-body shape, the C1850 21 24 breakup cross section is accurate to within 25 %. C1850 21 25 STATUS (CURVE) Fig. 6, page 125. C1850 21 26 ENDBIB 24 0 C1850 21 27 COMMON 2 3 C1850 21 28 EN ANG C1850 21 29 MEV ADEG C1850 21 30 6.3 15.0 C1850 21 31 ENDCOMMON 3 0 C1850 21 32 DATA 3 96 C1850 21 33 E-CM DATA-CM DATA-ERR C1850 21 34 MEV MB/SR/MEV MB/SR/MEV C1850 21 35 0.832 1.270E+01 8.042E-01 C1850 21 36 0.885 1.230E+01 C1850 21 37 0.917 1.425E+01 C1850 21 38 0.960 1.368E+01 C1850 21 39 0.993 1.314E+01 C1850 21 40 1.041 1.438E+01 C1850 21 41 1.083 1.486E+01 C1850 21 42 1.111 1.561E+01 C1850 21 43 1.163 1.980E+01 C1850 21 44 1.200 2.884E+01 C1850 21 45 1.246 4.378E+01 C1850 21 46 1.303 4.832E+01 C1850 21 47 1.322 3.812E+01 C1850 21 48 1.371 2.554E+01 C1850 21 49 1.424 1.490E+01 C1850 21 50 1.463 1.128E+01 C1850 21 51 1.496 8.687E+00 7.463E-01 C1850 21 52 1.534 8.833E+00 C1850 21 53 1.625 6.531E+00 C1850 21 54 1.668 5.457E+00 C1850 21 55 1.753 5.073E+00 C1850 21 56 1.801 4.103E+00 C1850 21 57 1.844 3.844E+00 C1850 21 58 1.872 4.207E+00 C1850 21 59 1.915 3.458E+00 C1850 21 60 1.958 3.663E+00 C1850 21 61 1.991 3.755E+00 5.401E-01 C1850 21 62 2.053 3.695E+00 C1850 21 63 2.086 3.519E+00 C1850 21 64 2.138 3.638E+00 C1850 21 65 2.218 3.854E+00 C1850 21 66 2.223 3.409E+00 C1850 21 67 2.257 2.992E+00 C1850 21 68 2.280 3.553E+00 C1850 21 69 2.294 3.763E+00 C1850 21 70 2.318 3.612E+00 C1850 21 71 2.333 3.018E+00 C1850 21 72 2.347 3.275E+00 C1850 21 73 2.352 2.781E+00 C1850 21 74 2.389 3.044E+00 C1850 21 75 2.390 2.737E+00 C1850 21 76 2.422 3.414E+00 C1850 21 77 2.428 2.671E+00 C1850 21 78 2.456 2.783E+00 C1850 21 79 2.479 3.500E+00 C1850 21 80 2.489 2.853E+00 C1850 21 81 2.490 2.307E+00 C1850 21 82 2.508 2.673E+00 4.763E-01 C1850 21 83 2.537 2.652E+00 C1850 21 84 2.565 3.023E+00 C1850 21 85 2.579 2.546E+00 C1850 21 86 2.589 2.059E+00 C1850 21 87 2.622 2.927E+00 C1850 21 88 2.631 2.568E+00 C1850 21 89 2.655 2.764E+00 C1850 21 90 2.669 2.880E+00 C1850 21 91 2.684 2.387E+00 C1850 21 92 2.722 2.387E+00 C1850 21 93 2.741 2.218E+00 C1850 21 94 2.756 1.680E+00 C1850 21 95 2.760 1.868E+00 C1850 21 96 2.779 2.255E+00 C1850 21 97 2.793 2.028E+00 C1850 21 98 2.816 2.408E+00 C1850 21 99 2.840 2.275E+00 C1850 21 100 2.869 1.824E+00 C1850 21 101 2.878 1.980E+00 C1850 21 102 2.883 2.097E+00 C1850 21 103 2.944 2.511E+00 C1850 21 104 2.960 1.213E+00 C1850 21 105 2.983 1.767E+00 C1850 21 106 3.020 1.950E+00 C1850 21 107 3.049 1.812E+00 C1850 21 108 3.073 1.783E+00 C1850 21 109 3.086 2.279E+00 C1850 21 110 3.115 2.279E+00 C1850 21 111 3.143 2.598E+00 C1850 21 112 3.165 5.935E+00 C1850 21 113 3.197 7.342E+00 C1850 21 114 3.206 1.035E+01 C1850 21 115 3.229 1.448E+01 C1850 21 116 3.247 1.944E+01 C1850 21 117 3.289 2.526E+01 C1850 21 118 3.303 3.049E+01 C1850 21 119 3.374 3.681E+01 2.613E+00 C1850 21 120 3.412 2.953E+01 C1850 21 121 3.431 2.743E+01 C1850 21 122 3.513 1.404E+01 C1850 21 123 3.547 9.562E+00 C1850 21 124 3.563 5.179E+00 C1850 21 125 3.612 3.020E+00 C1850 21 126 3.642 1.532E+00 C1850 21 127 3.667 6.990E-01 C1850 21 128 3.687 4.315E-01 C1850 21 129 3.703 1.952E-01 C1850 21 130 3.740 2.686E-01 C1850 21 131 ENDDATA 98 0 C1850 21 132 ENDSUBENT 131 0 C1850 2199999 SUBENT C1850022 20180315 C174C1850 22 1 BIB 7 24 C1850 22 2 REACTION (4-BE-9(P,X)0-NN-1,,DA/DE) C1850 22 3 SAMPLE A 1.28 mg/cm2 Be target evaporated on a 0.5 mm thick C1850 22 4 tantalum plate which was thick enough to stop the C1850 22 5 proton beam. C1850 22 6 DETECTOR (SCIN) The neutron detectors, consisting of 5 x 5 cm C1850 22 7 plastic scintillators mounted on RCA-6655 C1850 22 8 photomultipliers, were positioned, at 15 degree C1850 22 9 angular intervals in a well collimated and shielded C1850 22 10 geometry. C1850 22 11 METHOD (TOF) The neutron spectra were observed using time-of- C1850 22 12 flight techniques. A flight-path of about 10 m was C1850 22 13 chosen as an optimum considering neutron intensities C1850 22 14 and resolution of the experimental equipment. C1850 22 15 REL-REF (M,,J.D.Anderson+,J,NIM,15,178,1962) C1850 22 16 ERR-ANALYS (DATA-ERR) The absolute differential cross sections C1850 22 17 for the ground state group are accurate to within C1850 22 18 about 25%. The large uncertainty is due to the fact C1850 22 19 that the usual precautions with regard to charge C1850 22 20 collection have not been carefully observed since the C1850 22 21 main emphasis in this experiment was on energy C1850 22 22 spectra. In those cases where the continuous spectra C1850 22 23 are well described by the four-body shape, the C1850 22 24 breakup cross section is accurate to within 25 %. C1850 22 25 STATUS (CURVE) Fig. 6, page 125. C1850 22 26 ENDBIB 24 0 C1850 22 27 COMMON 2 3 C1850 22 28 EN ANG C1850 22 29 MEV ADEG C1850 22 30 6.3 45.0 C1850 22 31 ENDCOMMON 3 0 C1850 22 32 DATA 3 80 C1850 22 33 E-CM DATA-CM DATA-ERR C1850 22 34 MEV MB/SR/MEV MB/SR/MEV C1850 22 35 1.004 9.106E+00 1.314E+00 C1850 22 36 1.122 1.255E+01 C1850 22 37 1.169 1.528E+01 C1850 22 38 1.201 2.304E+01 C1850 22 39 1.309 3.201E+01 3.237E+00 C1850 22 40 1.348 2.630E+01 C1850 22 41 1.391 1.582E+01 C1850 22 42 1.430 1.094E+01 C1850 22 43 1.473 8.625E+00 C1850 22 44 1.516 7.323E+00 7.404E-01 C1850 22 45 1.607 6.168E+00 C1850 22 46 1.702 6.223E+00 C1850 22 47 1.735 5.196E+00 C1850 22 48 1.792 4.376E+00 C1850 22 49 1.826 4.270E+00 C1850 22 50 1.859 4.487E+00 C1850 22 51 1.915 4.526E+00 C1850 22 52 1.953 4.640E+00 C1850 22 53 2.015 4.071E+00 3.815E-01 C1850 22 54 2.058 3.876E+00 C1850 22 55 2.095 4.421E+00 C1850 22 56 2.143 3.815E+00 C1850 22 57 2.181 4.042E+00 C1850 22 58 2.229 3.634E+00 C1850 22 59 2.271 4.011E+00 C1850 22 60 2.323 3.637E+00 C1850 22 61 2.366 3.138E+00 C1850 22 62 2.452 2.917E+00 C1850 22 63 2.486 2.172E+00 C1850 22 64 2.514 2.172E+00 5.014E-01 C1850 22 65 2.542 3.091E+00 C1850 22 66 2.561 2.085E+00 C1850 22 67 2.575 2.848E+00 C1850 22 68 2.613 2.668E+00 C1850 22 69 2.632 2.321E+00 C1850 22 70 2.655 3.068E+00 C1850 22 71 2.694 2.380E+00 C1850 22 72 2.694 1.831E+00 C1850 22 73 2.708 2.020E+00 C1850 22 74 2.732 1.715E+00 C1850 22 75 2.741 2.158E+00 C1850 22 76 2.761 1.816E+00 C1850 22 77 2.784 2.158E+00 C1850 22 78 2.794 1.893E+00 C1850 22 79 2.823 1.581E+00 C1850 22 80 2.842 1.493E+00 C1850 22 81 2.855 1.909E+00 C1850 22 82 2.878 2.422E+00 C1850 22 83 2.898 1.990E+00 C1850 22 84 2.927 1.760E+00 C1850 22 85 2.945 1.789E+00 C1850 22 86 2.968 2.384E+00 C1850 22 87 2.997 2.179E+00 3.747E-01 C1850 22 88 3.026 1.880E+00 C1850 22 89 3.044 2.253E+00 C1850 22 90 3.087 1.960E+00 C1850 22 91 3.096 2.406E+00 C1850 22 92 3.101 2.634E+00 C1850 22 93 3.115 2.426E+00 C1850 22 94 3.129 3.129E+00 C1850 22 95 3.152 4.874E+00 C1850 22 96 3.179 6.390E+00 C1850 22 97 3.217 7.229E+00 C1850 22 98 3.249 1.273E+01 C1850 22 99 3.272 1.739E+01 C1850 22 100 3.290 2.050E+01 C1850 22 101 3.351 3.355E+01 C1850 22 102 3.370 3.672E+01 C1850 22 103 3.393 3.383E+01 C1850 22 104 3.412 3.584E+01 3.624E+00 C1850 22 105 3.460 3.276E+01 C1850 22 106 3.465 2.826E+01 C1850 22 107 3.494 2.459E+01 C1850 22 108 3.523 1.923E+01 C1850 22 109 3.538 1.351E+01 C1850 22 110 3.596 5.904E+00 C1850 22 111 3.641 2.687E+00 C1850 22 112 3.647 1.656E+00 C1850 22 113 3.681 1.136E+00 C1850 22 114 3.723 1.155E+00 C1850 22 115 ENDDATA 82 0 C1850 22 116 ENDSUBENT 115 0 C1850 2299999 SUBENT C1850023 20180315 C174C1850 23 1 BIB 7 24 C1850 23 2 REACTION (3-LI-6(A,X)0-NN-1,,DA/DE) C1850 23 3 SAMPLE (3-LI-6,ENR=0.93) a 1.3 mg/cm2 Li6 target (93% C1850 23 4 enriched) evaporated on a gold backing about 0.25 mm C1850 23 5 thick. C1850 23 6 DETECTOR (SCIN) The neutron detectors, consisting of 5 x 5 cm C1850 23 7 plastic scintillators mounted on RCA-6655 C1850 23 8 photomultipliers, were positioned, at 15 degree C1850 23 9 angular intervals in a well collimated and shielded C1850 23 10 geometry. C1850 23 11 METHOD (TOF) The neutron spectra were observed using time-of- C1850 23 12 flight techniques. A flight-path of about 10 m was C1850 23 13 chosen as an optimum considering neutron intensities C1850 23 14 and resolution of the experimental equipment. C1850 23 15 REL-REF (M,,J.D.Anderson+,J,NIM,15,178,1962) C1850 23 16 ERR-ANALYS (DATA-ERR) The absolute differential cross sections C1850 23 17 for the ground state group are accurate to within C1850 23 18 about 25%. The large uncertainty is due to the fact C1850 23 19 that the usual precautions with regard to charge C1850 23 20 collection have not been carefully observed since the C1850 23 21 main emphasis in this experiment was on energy C1850 23 22 spectra. In those cases where the continuous spectra C1850 23 23 are well described by the four-body shape, the C1850 23 24 breakup cross section is accurate to within 25 %. C1850 23 25 STATUS (CURVE) Fig. 7, page 126. C1850 23 26 ENDBIB 24 0 C1850 23 27 COMMON 2 3 C1850 23 28 EN ANG C1850 23 29 MEV ADEG C1850 23 30 14.4 15.0 C1850 23 31 ENDCOMMON 3 0 C1850 23 32 DATA 3 122 C1850 23 33 E-CM DATA-CM DATA-ERR C1850 23 34 MEV MB/SR/MEV MB/SR/MEV C1850 23 35 0.166 2.344E+00 C1850 23 36 0.181 2.775E+00 C1850 23 37 0.217 3.369E+00 C1850 23 38 0.260 4.302E+00 C1850 23 39 0.304 4.450E+00 C1850 23 40 0.304 3.988E+00 C1850 23 41 0.325 4.160E+00 C1850 23 42 0.354 4.056E+00 C1850 23 43 0.383 4.302E+00 C1850 23 44 0.412 4.056E+00 C1850 23 45 0.427 4.526E+00 C1850 23 46 0.484 3.954E+00 C1850 23 47 0.520 4.883E+00 C1850 23 48 0.535 3.514E+00 C1850 23 49 0.542 4.160E+00 C1850 23 50 0.542 3.855E+00 C1850 23 51 0.564 3.285E+00 C1850 23 52 0.586 4.966E+00 C1850 23 53 0.586 3.791E+00 C1850 23 54 0.614 4.090E+00 C1850 23 55 0.622 4.266E+00 C1850 23 56 0.629 3.397E+00 C1850 23 57 0.629 3.759E+00 C1850 23 58 0.636 3.257E+00 C1850 23 59 0.658 3.484E+00 C1850 23 60 0.665 2.968E+00 C1850 23 61 0.665 3.988E+00 C1850 23 62 0.672 2.798E+00 C1850 23 63 0.687 3.791E+00 C1850 23 64 0.694 2.616E+00 C1850 23 65 0.708 3.696E+00 C1850 23 66 0.730 3.514E+00 C1850 23 67 0.737 3.791E+00 C1850 23 68 0.737 4.266E+00 C1850 23 69 0.773 3.514E+00 C1850 23 70 0.781 4.266E+00 C1850 23 71 0.795 3.312E+00 C1850 23 72 0.817 3.514E+00 C1850 23 73 0.817 3.921E+00 C1850 23 74 0.824 3.759E+00 C1850 23 75 0.846 4.125E+00 C1850 23 76 0.846 4.450E+00 C1850 23 77 0.882 3.988E+00 C1850 23 78 0.889 4.642E+00 C1850 23 79 0.896 3.123E+00 C1850 23 80 0.925 4.339E+00 C1850 23 81 0.947 5.008E+00 C1850 23 82 0.983 4.564E+00 C1850 23 83 1.005 4.230E+00 C1850 23 84 1.019 4.375E+00 C1850 23 85 1.041 4.883E+00 5.438E-01 C1850 23 86 1.077 4.302E+00 C1850 23 87 1.106 4.266E+00 C1850 23 88 1.113 3.634E+00 C1850 23 89 1.128 3.921E+00 C1850 23 90 1.157 4.603E+00 C1850 23 91 1.178 3.312E+00 C1850 23 92 1.200 4.160E+00 C1850 23 93 1.200 3.888E+00 C1850 23 94 1.229 4.603E+00 C1850 23 95 1.287 4.842E+00 C1850 23 96 1.301 3.988E+00 C1850 23 97 1.316 4.603E+00 C1850 23 98 1.316 3.823E+00 C1850 23 99 1.345 3.514E+00 C1850 23 100 1.366 3.791E+00 C1850 23 101 1.388 3.954E+00 C1850 23 102 1.388 3.604E+00 C1850 23 103 1.424 3.791E+00 C1850 23 104 1.453 3.544E+00 C1850 23 105 1.475 3.176E+00 C1850 23 106 1.489 3.888E+00 C1850 23 107 1.525 3.285E+00 C1850 23 108 1.547 2.728E+00 1.994E-01 C1850 23 109 1.576 2.919E+00 C1850 23 110 1.605 2.572E+00 C1850 23 111 1.612 2.728E+00 C1850 23 112 1.634 2.305E+00 C1850 23 113 1.648 2.508E+00 C1850 23 114 1.684 2.344E+00 C1850 23 115 1.720 2.228E+00 C1850 23 116 1.771 2.364E+00 C1850 23 117 1.807 2.822E+00 C1850 23 118 1.843 1.964E+00 C1850 23 119 1.858 2.154E+00 C1850 23 120 1.880 1.805E+00 C1850 23 121 1.894 2.065E+00 C1850 23 122 1.923 2.247E+00 C1850 23 123 1.952 2.048E+00 C1850 23 124 1.988 2.247E+00 C1850 23 125 2.039 1.980E+00 C1850 23 126 2.096 1.659E+00 C1850 23 127 2.176 1.026E+00 C1850 23 128 2.292 8.167E-01 C1850 23 129 2.443 4.450E-01 C1850 23 130 2.559 3.921E-01 4.367E-02 C1850 23 131 2.704 3.604E-01 C1850 23 132 2.812 3.096E-01 C1850 23 133 2.949 3.257E-01 C1850 23 134 2.993 2.572E-01 C1850 23 135 3.065 2.508E-01 3.532E-02 C1850 23 136 3.202 2.487E-01 C1850 23 137 3.318 3.019E-01 C1850 23 138 3.361 3.855E-01 C1850 23 139 3.427 4.681E-01 C1850 23 140 3.484 3.397E-01 6.919E-02 C1850 23 141 3.528 5.136E-01 C1850 23 142 3.607 5.312E-01 C1850 23 143 3.665 6.958E-01 C1850 23 144 3.701 8.962E-01 C1850 23 145 3.752 1.061E+00 C1850 23 146 3.817 1.043E+00 C1850 23 147 3.867 1.288E+00 C1850 23 148 4.005 1.245E+00 1.007E-01 C1850 23 149 4.048 1.310E+00 C1850 23 150 4.135 1.194E+00 C1850 23 151 4.193 8.886E-01 C1850 23 152 4.323 7.963E-01 C1850 23 153 4.431 4.842E-01 C1850 23 154 4.561 2.798E-01 C1850 23 155 4.742 2.173E-01 C1850 23 156 4.829 1.898E-01 C1850 23 157 ENDDATA 124 0 C1850 23 158 ENDSUBENT 157 0 C1850 2399999 SUBENT C1850024 20180315 C174C1850 24 1 BIB 7 24 C1850 24 2 REACTION (3-LI-6(A,X)0-NN-1,,DA/DE) C1850 24 3 SAMPLE (3-LI-6,ENR=0.93) a 1.3 mg/cm2 Li6 target (93% C1850 24 4 enriched) evaporated on a gold backing about 0.25 mm C1850 24 5 thick. C1850 24 6 DETECTOR (SCIN) The neutron detectors, consisting of 5 x 5 cm C1850 24 7 plastic scintillators mounted on RCA-6655 C1850 24 8 photomultipliers, were positioned, at 15 degree C1850 24 9 angular intervals in a well collimated and shielded C1850 24 10 geometry. C1850 24 11 METHOD (TOF) The neutron spectra were observed using time-of- C1850 24 12 flight techniques. A flight-path of about 10 m was C1850 24 13 chosen as an optimum considering neutron intensities C1850 24 14 and resolution of the experimental equipment. C1850 24 15 REL-REF (M,,J.D.Anderson+,J,NIM,15,178,1962) C1850 24 16 ERR-ANALYS (DATA-ERR) The absolute differential cross sections C1850 24 17 for the ground state group are accurate to within C1850 24 18 about 25%. The large uncertainty is due to the fact C1850 24 19 that the usual precautions with regard to charge C1850 24 20 collection have not been carefully observed since the C1850 24 21 main emphasis in this experiment was on energy C1850 24 22 spectra. In those cases where the continuous spectra C1850 24 23 are well described by the four-body shape, the C1850 24 24 breakup cross section is accurate to within 25 %. C1850 24 25 STATUS (CURVE) Fig. 7, page 126. C1850 24 26 ENDBIB 24 0 C1850 24 27 COMMON 2 3 C1850 24 28 EN ANG C1850 24 29 MEV ADEG C1850 24 30 14.4 30.0 C1850 24 31 ENDCOMMON 3 0 C1850 24 32 DATA 3 120 C1850 24 33 E-CM DATA-CM DATA-ERR C1850 24 34 MEV MB/SR/MEV MB/SR/MEV C1850 24 35 0.239 1.077E+00 C1850 24 36 0.267 1.281E+00 C1850 24 37 0.289 1.872E+00 C1850 24 38 0.311 2.208E+00 C1850 24 39 0.369 2.320E+00 C1850 24 40 0.369 2.737E+00 C1850 24 41 0.398 3.149E+00 C1850 24 42 0.419 3.448E+00 C1850 24 43 0.434 3.047E+00 C1850 24 44 0.463 3.255E+00 C1850 24 45 0.484 3.477E+00 C1850 24 46 0.506 3.282E+00 C1850 24 47 0.549 2.924E+00 C1850 24 48 0.607 3.072E+00 C1850 24 49 0.614 3.336E+00 C1850 24 50 0.643 2.829E+00 C1850 24 51 0.651 2.972E+00 C1850 24 52 0.716 2.997E+00 C1850 24 53 0.752 2.245E+00 C1850 24 54 0.766 2.829E+00 C1850 24 55 0.773 2.948E+00 C1850 24 56 0.788 2.499E+00 C1850 24 57 0.810 3.364E+00 C1850 24 58 0.817 2.398E+00 C1850 24 59 0.824 2.852E+00 C1850 24 60 0.831 2.190E+00 C1850 24 61 0.846 2.541E+00 C1850 24 62 0.875 2.924E+00 C1850 24 63 0.875 3.255E+00 C1850 24 64 0.882 2.340E+00 C1850 24 65 0.896 3.506E+00 C1850 24 66 0.904 2.208E+00 C1850 24 67 0.940 2.714E+00 C1850 24 68 0.947 2.900E+00 C1850 24 69 0.961 3.255E+00 C1850 24 70 1.027 2.972E+00 2.355E-01 C1850 24 71 1.041 2.499E+00 C1850 24 72 1.063 2.714E+00 C1850 24 73 1.070 3.282E+00 C1850 24 74 1.077 3.839E+00 C1850 24 75 1.084 2.852E+00 C1850 24 76 1.106 3.047E+00 C1850 24 77 1.128 3.684E+00 C1850 24 78 1.135 2.997E+00 C1850 24 79 1.149 2.805E+00 C1850 24 80 1.157 3.282E+00 C1850 24 81 1.186 2.997E+00 C1850 24 82 1.193 2.438E+00 C1850 24 83 1.229 3.282E+00 C1850 24 84 1.236 2.137E+00 C1850 24 85 1.243 2.782E+00 C1850 24 86 1.251 2.418E+00 C1850 24 87 1.272 2.626E+00 C1850 24 88 1.294 2.997E+00 C1850 24 89 1.323 2.876E+00 C1850 24 90 1.330 2.670E+00 C1850 24 91 1.337 3.072E+00 C1850 24 92 1.359 3.448E+00 C1850 24 93 1.366 2.876E+00 C1850 24 94 1.373 2.398E+00 C1850 24 95 1.388 2.737E+00 C1850 24 96 1.402 3.022E+00 C1850 24 97 1.410 2.418E+00 C1850 24 98 1.431 3.149E+00 C1850 24 99 1.453 2.479E+00 1.775E-01 C1850 24 100 1.489 2.900E+00 C1850 24 101 1.518 2.379E+00 C1850 24 102 1.540 2.520E+00 C1850 24 103 1.547 2.438E+00 C1850 24 104 1.569 2.301E+00 C1850 24 105 1.590 2.208E+00 C1850 24 106 1.605 2.067E+00 C1850 24 107 1.627 2.924E+00 C1850 24 108 1.655 2.208E+00 C1850 24 109 1.684 1.668E+00 C1850 24 110 1.713 2.000E+00 C1850 24 111 1.735 1.724E+00 C1850 24 112 1.749 1.346E+00 C1850 24 113 1.757 1.498E+00 C1850 24 114 1.793 1.474E+00 C1850 24 115 1.829 1.710E+00 C1850 24 116 1.865 1.281E+00 C1850 24 117 1.923 1.919E+00 C1850 24 118 1.945 1.523E+00 C1850 24 119 1.988 2.245E+00 C1850 24 120 1.995 2.670E+00 1.706E-01 C1850 24 121 2.060 2.759E+00 1.975E-01 C1850 24 122 2.067 1.826E+00 C1850 24 123 2.082 1.654E+00 C1850 24 124 2.118 2.102E+00 C1850 24 125 2.161 2.282E+00 C1850 24 126 2.190 1.826E+00 C1850 24 127 2.270 1.357E+00 C1850 24 128 2.465 5.657E-01 C1850 24 129 2.465 6.456E-01 C1850 24 130 2.588 5.209E-01 7.191E-02 C1850 24 131 2.718 2.084E-01 C1850 24 132 2.841 1.724E-01 C1850 24 133 2.971 2.418E-01 C1850 24 134 3.094 1.935E-01 3.477E-02 C1850 24 135 3.217 2.101E-01 C1850 24 136 3.361 1.983E-01 C1850 24 137 3.463 1.811E-01 C1850 24 138 3.643 2.562E-01 5.453E-02 C1850 24 139 3.672 4.641E-01 C1850 24 140 3.737 2.972E-01 C1850 24 141 3.846 6.403E-01 C1850 24 142 3.925 1.438E+00 C1850 24 143 4.005 1.511E+00 C1850 24 144 4.041 1.842E+00 C1850 24 145 4.084 2.340E+00 C1850 24 146 4.157 2.208E+00 C1850 24 147 4.229 2.359E+00 1.689E-01 C1850 24 148 4.287 2.154E+00 C1850 24 149 4.352 2.137E+00 C1850 24 150 4.402 1.682E+00 C1850 24 151 4.482 1.068E+00 C1850 24 152 4.598 4.836E-01 C1850 24 153 4.670 2.828E-01 C1850 24 154 4.749 1.150E-01 C1850 24 155 ENDDATA 122 0 C1850 24 156 ENDSUBENT 155 0 C1850 2499999 SUBENT C1850025 20180315 C174C1850 25 1 BIB 7 24 C1850 25 2 REACTION (3-LI-6(A,X)0-NN-1,,DA/DE) C1850 25 3 SAMPLE (3-LI-6,ENR=0.93) a 1.3 mg/cm2 Li6 target (93% C1850 25 4 enriched) evaporated on a gold backing about 0.25 mm C1850 25 5 thick. C1850 25 6 DETECTOR (SCIN) The neutron detectors, consisting of 5 x 5 cm C1850 25 7 plastic scintillators mounted on RCA-6655 C1850 25 8 photomultipliers, were positioned, at 15 degree C1850 25 9 angular intervals in a well collimated and shielded C1850 25 10 geometry. C1850 25 11 METHOD (TOF) The neutron spectra were observed using time-of- C1850 25 12 flight techniques. A flight-path of about 10 m was C1850 25 13 chosen as an optimum considering neutron intensities C1850 25 14 and resolution of the experimental equipment. C1850 25 15 REL-REF (M,,J.D.Anderson+,J,NIM,15,178,1962) C1850 25 16 ERR-ANALYS (DATA-ERR) The absolute differential cross sections C1850 25 17 for the ground state group are accurate to within C1850 25 18 about 25%. The large uncertainty is due to the fact C1850 25 19 that the usual precautions with regard to charge C1850 25 20 collection have not been carefully observed since the C1850 25 21 main emphasis in this experiment was on energy C1850 25 22 spectra. In those cases where the continuous spectra C1850 25 23 are well described by the four-body shape, the C1850 25 24 breakup cross section is accurate to within 25 %. C1850 25 25 STATUS (CURVE) Fig. 7, page 126. C1850 25 26 ENDBIB 24 0 C1850 25 27 COMMON 2 3 C1850 25 28 EN ANG C1850 25 29 MEV ADEG C1850 25 30 14.4 45.0 C1850 25 31 ENDCOMMON 3 0 C1850 25 32 DATA 3 98 C1850 25 33 E-CM DATA-CM DATA-ERR C1850 25 34 MEV MB/SR/MEV MB/SR/MEV C1850 25 35 0.911 2.456E+00 C1850 25 36 0.947 2.542E+00 C1850 25 37 0.998 2.586E+00 2.531E-01 C1850 25 38 1.084 2.141E+00 C1850 25 39 1.084 2.498E+00 C1850 25 40 1.092 3.176E+00 C1850 25 41 1.092 1.759E+00 C1850 25 42 1.113 2.675E+00 C1850 25 43 1.120 2.939E+00 C1850 25 44 1.135 2.052E+00 C1850 25 45 1.157 3.230E+00 C1850 25 46 1.171 2.498E+00 C1850 25 47 1.214 2.698E+00 C1850 25 48 1.222 3.967E+00 C1850 25 49 1.229 2.520E+00 C1850 25 50 1.236 3.203E+00 C1850 25 51 1.258 3.460E+00 C1850 25 52 1.272 2.914E+00 C1850 25 53 1.287 2.653E+00 C1850 25 54 1.308 3.176E+00 C1850 25 55 1.308 3.042E+00 C1850 25 56 1.330 2.865E+00 C1850 25 57 1.345 3.095E+00 C1850 25 58 1.345 2.414E+00 C1850 25 59 1.359 2.254E+00 C1850 25 60 1.366 2.675E+00 C1850 25 61 1.395 2.456E+00 C1850 25 62 1.402 2.698E+00 C1850 25 63 1.410 3.611E+00 C1850 25 64 1.417 2.160E+00 C1850 25 65 1.431 2.890E+00 C1850 25 66 1.439 2.520E+00 C1850 25 67 1.475 2.216E+00 C1850 25 68 1.482 2.105E+00 C1850 25 69 1.496 3.286E+00 C1850 25 70 1.511 2.564E+00 C1850 25 71 1.540 2.236E+00 2.361E-01 C1850 25 72 1.583 2.236E+00 C1850 25 73 1.612 1.670E+00 C1850 25 74 1.641 2.160E+00 C1850 25 75 1.648 1.852E+00 C1850 25 76 1.677 2.314E+00 C1850 25 77 1.699 1.685E+00 C1850 25 78 1.728 1.949E+00 C1850 25 79 1.728 2.105E+00 C1850 25 80 1.771 2.456E+00 C1850 25 81 1.793 1.949E+00 C1850 25 82 1.829 2.564E+00 C1850 25 83 1.843 2.141E+00 C1850 25 84 1.851 3.314E+00 C1850 25 85 1.858 2.939E+00 C1850 25 86 1.901 3.121E+00 2.070E-01 C1850 25 87 1.908 3.900E+00 C1850 25 88 1.930 2.722E+00 C1850 25 89 1.966 3.068E+00 C1850 25 90 1.981 2.675E+00 C1850 25 91 2.046 3.176E+00 3.597E-01 C1850 25 92 2.089 2.675E+00 C1850 25 93 2.104 2.456E+00 C1850 25 94 2.154 1.744E+00 C1850 25 95 2.169 1.432E+00 C1850 25 96 2.219 1.729E+00 C1850 25 97 2.255 1.534E+00 C1850 25 98 2.292 7.667E-01 C1850 25 99 2.451 5.040E-01 C1850 25 100 2.566 5.633E-01 5.514E-02 C1850 25 101 2.704 4.433E-01 C1850 25 102 2.812 4.747E-01 C1850 25 103 3.072 3.016E-01 2.717E-02 C1850 25 104 3.217 2.235E-01 C1850 25 105 3.318 2.816E-01 C1850 25 106 3.448 3.174E-01 C1850 25 107 3.535 2.865E-01 2.128E-02 C1850 25 108 3.564 3.735E-01 C1850 25 109 3.564 3.548E-01 C1850 25 110 3.672 7.409E-01 C1850 25 111 3.745 7.098E-01 C1850 25 112 3.773 8.792E-01 C1850 25 113 3.839 8.868E-01 C1850 25 114 3.860 1.008E+00 C1850 25 115 3.904 1.715E+00 C1850 25 116 3.954 1.657E+00 C1850 25 117 3.990 2.052E+00 C1850 25 118 4.027 2.353E+00 C1850 25 119 4.106 2.414E+00 C1850 25 120 4.142 2.236E+00 C1850 25 121 4.193 2.478E+00 2.232E-01 C1850 25 122 4.316 2.070E+00 C1850 25 123 4.395 2.070E+00 C1850 25 124 4.439 1.670E+00 C1850 25 125 4.511 1.600E+00 C1850 25 126 4.576 1.166E+00 C1850 25 127 4.619 9.099E-01 C1850 25 128 4.670 5.040E-01 C1850 25 129 4.757 4.587E-01 C1850 25 130 4.814 2.607E-01 C1850 25 131 4.887 2.414E-01 C1850 25 132 4.930 1.520E-01 C1850 25 133 ENDDATA 100 0 C1850 25 134 ENDSUBENT 133 0 C1850 2599999 SUBENT C1850026 20180315 C174C1850 26 1 BIB 7 24 C1850 26 2 REACTION (3-LI-6(A,X)0-NN-1,,DA/DE) C1850 26 3 SAMPLE (3-LI-6,ENR=0.93) a 1.3 mg/cm2 Li6 target (93% C1850 26 4 enriched) evaporated on a gold backing about 0.25 mm C1850 26 5 thick. C1850 26 6 DETECTOR (SCIN) The neutron detectors, consisting of 5 x 5 cm C1850 26 7 plastic scintillators mounted on RCA-6655 C1850 26 8 photomultipliers, were positioned, at 15 degree C1850 26 9 angular intervals in a well collimated and shielded C1850 26 10 geometry. C1850 26 11 METHOD (TOF) The neutron spectra were observed using time-of- C1850 26 12 flight techniques. A flight-path of about 10 m was C1850 26 13 chosen as an optimum considering neutron intensities C1850 26 14 and resolution of the experimental equipment. C1850 26 15 REL-REF (M,,J.D.Anderson+,J,NIM,15,178,1962) C1850 26 16 ERR-ANALYS (DATA-ERR) The absolute differential cross sections C1850 26 17 for the ground state group are accurate to within C1850 26 18 about 25%. The large uncertainty is due to the fact C1850 26 19 that the usual precautions with regard to charge C1850 26 20 collection have not been carefully observed since the C1850 26 21 main emphasis in this experiment was on energy C1850 26 22 spectra. In those cases where the continuous spectra C1850 26 23 are well described by the four-body shape, the C1850 26 24 breakup cross section is accurate to within 25 %. C1850 26 25 STATUS (CURVE) Fig. 7, page 126. C1850 26 26 ENDBIB 24 0 C1850 26 27 COMMON 2 3 C1850 26 28 EN ANG C1850 26 29 MEV ADEG C1850 26 30 14.4 60.0 C1850 26 31 ENDCOMMON 3 0 C1850 26 32 DATA 3 82 C1850 26 33 E-CM DATA-CM DATA-ERR C1850 26 34 MEV MB/SR/MEV MB/SR/MEV C1850 26 35 0.983 2.708E+00 C1850 26 36 0.998 3.428E+00 C1850 26 37 1.034 3.047E+00 2.223E-01 C1850 26 38 1.055 2.708E+00 C1850 26 39 1.113 2.469E+00 C1850 26 40 1.193 2.731E+00 C1850 26 41 1.207 2.825E+00 C1850 26 42 1.251 3.073E+00 C1850 26 43 1.294 2.469E+00 C1850 26 44 1.337 2.731E+00 C1850 26 45 1.373 3.073E+00 C1850 26 46 1.424 3.099E+00 C1850 26 47 1.453 2.996E+00 C1850 26 48 1.511 2.139E+00 C1850 26 49 1.518 2.825E+00 2.061E-01 C1850 26 50 1.561 2.618E+00 C1850 26 51 1.576 2.777E+00 C1850 26 52 1.576 2.176E+00 C1850 26 53 1.590 3.151E+00 C1850 26 54 1.612 2.596E+00 C1850 26 55 1.619 1.901E+00 C1850 26 56 1.619 2.194E+00 C1850 26 57 1.648 2.448E+00 C1850 26 58 1.655 2.250E+00 C1850 26 59 1.670 2.663E+00 C1850 26 60 1.684 2.801E+00 C1850 26 61 1.684 2.194E+00 C1850 26 62 1.706 1.983E+00 C1850 26 63 1.706 1.607E+00 C1850 26 64 1.720 2.308E+00 C1850 26 65 1.720 1.763E+00 C1850 26 66 1.778 1.748E+00 C1850 26 67 1.778 2.139E+00 C1850 26 68 1.786 2.250E+00 C1850 26 69 1.814 2.176E+00 C1850 26 70 1.814 2.708E+00 C1850 26 71 1.822 2.897E+00 C1850 26 72 1.836 1.934E+00 C1850 26 73 1.843 1.748E+00 C1850 26 74 1.872 2.121E+00 C1850 26 75 1.880 2.825E+00 C1850 26 76 1.894 3.486E+00 C1850 26 77 1.908 2.596E+00 C1850 26 78 1.945 2.250E+00 C1850 26 79 1.945 5.179E+00 C1850 26 80 1.995 5.356E+00 C1850 26 81 2.060 4.091E+00 3.303E-01 C1850 26 82 2.096 4.376E+00 C1850 26 83 2.111 3.343E+00 C1850 26 84 2.161 4.196E+00 C1850 26 85 2.169 3.729E+00 C1850 26 86 2.219 3.343E+00 C1850 26 87 2.234 2.469E+00 C1850 26 88 2.357 1.477E+00 C1850 26 89 2.451 7.531E-01 C1850 26 90 2.559 6.102E-01 3.975E-02 C1850 26 91 2.696 6.694E-01 C1850 26 92 2.827 5.469E-01 C1850 26 93 2.957 6.206E-01 C1850 26 94 3.080 5.850E-01 5.622E-02 C1850 26 95 3.202 4.039E-01 C1850 26 96 3.325 4.394E-01 C1850 26 97 3.448 3.059E-01 C1850 26 98 3.578 5.070E-01 1.065E-01 C1850 26 99 3.651 5.378E-01 C1850 26 100 3.665 7.282E-01 C1850 26 101 3.716 5.704E-01 C1850 26 102 3.802 6.865E-01 C1850 26 103 3.853 7.659E-01 C1850 26 104 3.925 1.259E+00 C1850 26 105 3.961 2.176E+00 C1850 26 106 4.157 3.371E+00 C1850 26 107 4.193 2.825E+00 3.972E-01 C1850 26 108 4.301 2.754E+00 C1850 26 109 4.381 2.946E+00 C1850 26 110 4.395 2.000E+00 C1850 26 111 4.467 1.515E+00 C1850 26 112 4.511 1.177E+00 C1850 26 113 4.554 8.764E-01 C1850 26 114 4.590 5.469E-01 C1850 26 115 4.641 3.776E-01 C1850 26 116 4.699 1.123E-01 C1850 26 117 ENDDATA 84 0 C1850 26 118 ENDSUBENT 117 0 C1850 2699999 SUBENT C1850027 20180317 C174C1850 27 1 BIB 7 24 C1850 27 2 REACTION (3-LI-6(A,X)0-NN-1,,DA/DE) C1850 27 3 SAMPLE (3-LI-6,ENR=0.93) a 1.3 mg/cm2 Li6 target (93% C1850 27 4 enriched) evaporated on a gold backing about 0.25 mm C1850 27 5 thick. C1850 27 6 DETECTOR (SCIN) The neutron detectors, consisting of 5 x 5 cm C1850 27 7 plastic scintillators mounted on RCA-6655 C1850 27 8 photomultipliers, were positioned, at 15 degree C1850 27 9 angular intervals in a well collimated and shielded C1850 27 10 geometry. C1850 27 11 METHOD (TOF) The neutron spectra were observed using time-of- C1850 27 12 flight techniques. A flight-path of about 10 m was C1850 27 13 chosen as an optimum considering neutron intensities C1850 27 14 and resolution of the experimental equipment. C1850 27 15 REL-REF (M,,J.D.Anderson+,J,NIM,15,178,1962) C1850 27 16 ERR-ANALYS (DATA-ERR) The absolute differential cross sections C1850 27 17 for the ground state group are accurate to within C1850 27 18 about 25%. The large uncertainty is due to the fact C1850 27 19 that the usual precautions with regard to charge C1850 27 20 collection have not been carefully observed since the C1850 27 21 main emphasis in this experiment was on energy C1850 27 22 spectra. In those cases where the continuous spectra C1850 27 23 are well described by the four-body shape, the C1850 27 24 breakup cross section is accurate to within 25 %. C1850 27 25 STATUS (CURVE) Fig. 7, page 126. C1850 27 26 ENDBIB 24 0 C1850 27 27 COMMON 2 3 C1850 27 28 EN ANG C1850 27 29 MEV ADEG C1850 27 30 14.4 75.0 C1850 27 31 ENDCOMMON 3 0 C1850 27 32 DATA 3 44 C1850 27 33 E-CM DATA-CM DATA-ERR C1850 27 34 MEV MB/SR/MEV MB/SR/MEV C1850 27 35 1.569 1.951E+00 1.985E-01 C1850 27 36 1.648 2.033E+00 C1850 27 37 1.663 1.486E+00 C1850 27 38 1.728 1.498E+00 C1850 27 39 1.764 1.696E+00 C1850 27 40 1.800 1.335E+00 C1850 27 41 1.836 1.426E+00 C1850 27 42 1.880 1.486E+00 C1850 27 43 1.901 1.935E+00 C1850 27 44 1.952 2.137E+00 C1850 27 45 2.002 2.227E+00 2.100E-01 C1850 27 46 2.060 2.924E+00 C1850 27 47 2.140 2.479E+00 C1850 27 48 2.205 2.459E+00 C1850 27 49 2.227 1.767E+00 C1850 27 50 2.306 8.340E-01 C1850 27 51 2.465 5.995E-01 C1850 27 52 2.559 3.935E-01 9.873E-02 C1850 27 53 2.704 5.946E-01 C1850 27 54 2.834 2.033E-01 C1850 27 55 2.942 4.169E-01 C1850 27 56 3.080 2.379E-01 8.428E-02 C1850 27 57 3.210 2.948E-01 C1850 27 58 3.318 1.588E-01 C1850 27 59 3.441 3.364E-01 C1850 27 60 3.571 2.499E-01 8.036E-02 C1850 27 61 3.701 1.696E-01 C1850 27 62 3.810 1.812E-01 C1850 27 63 3.860 2.245E-01 C1850 27 64 3.875 2.852E-01 C1850 27 65 3.933 2.948E-01 C1850 27 66 3.954 1.160E+00 C1850 27 67 4.019 1.077E+00 C1850 27 68 4.041 1.812E+00 C1850 27 69 4.070 1.654E+00 C1850 27 70 4.106 2.190E+00 C1850 27 71 4.128 2.283E+00 C1850 27 72 4.178 2.102E+00 C1850 27 73 4.193 2.340E+00 2.380E-01 C1850 27 74 4.316 1.160E+00 C1850 27 75 4.359 6.955E-01 C1850 27 76 4.388 4.797E-01 C1850 27 77 4.431 3.123E-01 C1850 27 78 4.547 1.682E-01 C1850 27 79 ENDDATA 46 0 C1850 27 80 ENDSUBENT 79 0 C1850 2799999 SUBENT C1850028 20180315 C174C1850 28 1 BIB 4 8 C1850 28 2 REACTION (6-C-12(P,A)5-B-9,PAR,DA) C1850 28 3 ANALYSIS Authors say that the cs is "roughly constant" in this C1850 28 4 energy range 14.3 - 18.3 MeV. C1850 28 5 ERR-ANALYS (DATA-ERR) No details given C1850 28 6 STATUS (DEP,C1850003) C1850 28 7 (DEP,C1850004) C1850 28 8 (DEP,C1850005) C1850 28 9 (TABLE) page 123. C1850 28 10 ENDBIB 8 0 C1850 28 11 COMMON 5 3 C1850 28 12 EN-MIN EN-MAX ANG-MIN ANG-MAX E-LVL C1850 28 13 MEV MEV ADEG ADEG MEV C1850 28 14 14.3 18.3 86.0 90.0 0.0 C1850 28 15 ENDCOMMON 3 0 C1850 28 16 DATA 2 1 C1850 28 17 DATA DATA-ERR C1850 28 18 MB/SR MB/SR C1850 28 19 2.0 0.5 C1850 28 20 ENDDATA 3 0 C1850 28 21 ENDSUBENT 20 0 C1850 2899999 SUBENT C1850029 20180315 C174C1850 29 1 BIB 3 10 C1850 29 2 REACTION (4-BE-9(P,N)5-B-9,PAR,DA) C1850 29 3 EN-SEC (E-LVL,4-BE-9) C1850 29 4 STATUS (DEP,C1850016) C1850 29 5 (DEP,C1850017) C1850 29 6 (DEP,C1850018) C1850 29 7 (DEP,C1850019) C1850 29 8 (DEP,C1850020) C1850 29 9 (DEP,C1850021) C1850 29 10 (DEP,C1850022) C1850 29 11 (TABLE) page 126. C1850 29 12 ENDBIB 10 0 C1850 29 13 COMMON 5 3 C1850 29 14 EN-MIN EN-MAX ANG-MIN ANG-MAX E-LVL C1850 29 15 MEV MEV ADEG ADEG MEV C1850 29 16 6.3 7.4 3.0 105.0 1.7 C1850 29 17 ENDCOMMON 3 0 C1850 29 18 DATA 1 1 C1850 29 19 DATA-MAX C1850 29 20 MB/SR C1850 29 21 0.1 C1850 29 22 ENDDATA 3 0 C1850 29 23 ENDSUBENT 22 0 C1850 2999999 SUBENT C1850030 20180315 C174C1850 30 1 BIB 3 7 C1850 30 2 REACTION (3-LI-6(A,N)5-B-9,PAR,DA) C1850 30 3 ERR-ANALYS (DATA-ERR) No details given C1850 30 4 STATUS (DEP,C1850023) C1850 30 5 (DEP,C1850024) C1850 30 6 (DEP,C1850025) C1850 30 7 (DEP,C1850026) C1850 30 8 (TABLE) page 126. C1850 30 9 ENDBIB 7 0 C1850 30 10 COMMON 4 3 C1850 30 11 EN ANG-MIN ANG-MAX E-LVL C1850 30 12 MEV ADEG ADEG MEV C1850 30 13 14.4 15.0 60.0 0.0 C1850 30 14 ENDCOMMON 3 0 C1850 30 15 DATA 2 1 C1850 30 16 DATA DATA-ERR C1850 30 17 MB/SR MB/SR C1850 30 18 1.0 0.25 C1850 30 19 ENDDATA 3 0 C1850 30 20 ENDSUBENT 19 0 C1850 3099999 SUBENT C1850031 20180315 C174C1850 31 1 BIB 2 3 C1850 31 2 REACTION (3-LI-6(A,N)5-B-9,PAR,DA) C1850 31 3 STATUS (DEP,C1850027) C1850 31 4 (TABLE) page 126. C1850 31 5 ENDBIB 3 0 C1850 31 6 COMMON 3 3 C1850 31 7 EN ANG E-LVL C1850 31 8 MEV ADEG MEV C1850 31 9 14.4 75.0 0.0 C1850 31 10 ENDCOMMON 3 0 C1850 31 11 DATA 1 1 C1850 31 12 DATA C1850 31 13 MB/SR C1850 31 14 0.6 C1850 31 15 ENDDATA 3 0 C1850 31 16 ENDSUBENT 15 0 C1850 3199999 ENDENTRY 31 0 C185099999999