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