ENTRY C2880 20230106 C226C288000000001
SUBENT C2880001 20230106 C226C288000100001
BIB 7 17 C288000100002
TITLE 10Be(d,p)11Be and the 10Be(d,alpha)8Li Reactions C288000100003
AUTHOR (D.R.Goosman,R.W.Kavanagh) C288000100004
REFERENCE (J,PR/C,1,1939,1970) C288000100005
#doi:10.1103/PhysRevC.1.1939 C288000100006
INSTITUTE (1USACAL) C288000100007
SAMPLE (4-BE-10,ENR=0.05) A BeO target, 75+-8 microg/cm2 C288000100008
thick (1.36+- 0.35 microg/cm2 of 10Be), on a 5.7+- C288000100009
0.4-mg/cm2 Pt foil, was mounted on a stainless-steel C288000100010
holder and placed in a small chamber with the BeO C288000100011
upstream on the foil. Beryllium enriched to 5% in C288000100012
10Be has been extracted from neutron-irradiated C288000100013
carbon, and has been used for targets in nuclear C288000100014
spectroscopy. C288000100015
DETECTOR (SCIN) A plastic scintillator (Pilot B, 12.7 cm diam C288000100016
by 10.2 cm deep), to detect the beta-rays from the C288000100017
decay of 8Li and 11Be. C288000100018
HISTORY (20230106C) BP C288000100019
ENDBIB 17 0 C288000100020
NOCOMMON 0 0 C288000100021
ENDSUBENT 20 0 C288000199999
SUBENT C2880002 20230106 C226C288000200001
BIB 4 9 C288000200002
REACTION (4-BE-10(D,A)3-LI-8,,SIG) C288000200003
METHOD The curve results from data accumulated during two C288000200004
mean lives after target irradiation. Alpha particles C288000200005
populating both the ground and 0.98-MeV states of Li C288000200006
contribute to the yield. C288000200007
RAD-DET (3-LI-8,B) C288000200008
STATUS (CURVE,,D.R.Goosman+,J,PR/C,1,1939,1970) C288000200009
Fig. 2, upper curve, page 1940 of C288000200010
J,PR/C,1,1939,1970. C288000200011
ENDBIB 9 0 C288000200012
NOCOMMON 0 0 C288000200013
DATA 2 60 C288000200014
EN DATA C288000200015
MEV MB C288000200016
0.663 3.265E+00 C288000200017
0.683 3.719E+00 C288000200018
0.713 4.119E+00 C288000200019
0.737 5.076E+00 C288000200020
0.760 5.778E+00 C288000200021
0.790 6.070E+00 C288000200022
0.813 6.729E+00 C288000200023
0.837 7.865E+00 C288000200024
0.860 8.953E+00 C288000200025
0.887 1.046E+01 C288000200026
0.929 1.097E+01 C288000200027
0.952 1.317E+01 C288000200028
0.983 1.459E+01 C288000200029
1.009 1.660E+01 C288000200030
1.040 1.887E+01 C288000200031
1.055 1.986E+01 C288000200032
1.086 2.200E+01 C288000200033
1.109 2.439E+01 C288000200034
1.132 2.633E+01 C288000200035
1.163 2.917E+01 C288000200036
1.193 3.230E+01 C288000200037
1.213 3.489E+01 C288000200038
1.239 3.867E+01 C288000200039
1.270 3.956E+01 C288000200040
1.300 4.267E+01 C288000200041
1.323 4.255E+01 C288000200042
1.357 4.468E+01 C288000200043
1.384 4.573E+01 C288000200044
1.426 4.798E+01 C288000200045
1.460 4.778E+01 C288000200046
1.502 5.012E+01 C288000200047
1.540 4.990E+01 C288000200048
1.582 4.709E+01 C288000200049
1.646 4.672E+01 C288000200050
1.692 4.771E+01 C288000200051
1.733 4.624E+01 C288000200052
1.786 4.717E+01 C288000200053
1.840 4.687E+01 C288000200054
1.897 4.908E+01 C288000200055
1.950 4.877E+01 C288000200056
1.992 4.983E+01 C288000200057
2.049 5.358E+01 C288000200058
2.128 5.033E+01 C288000200059
2.193 4.737E+01 C288000200060
2.249 4.831E+01 C288000200061
2.306 4.798E+01 C288000200062
2.348 5.033E+01 C288000200063
2.405 5.270E+01 C288000200064
2.455 5.239E+01 C288000200065
2.496 5.353E+01 C288000200066
2.549 5.180E+01 C288000200067
2.614 5.419E+01 C288000200068
2.667 5.385E+01 C288000200069
2.717 5.496E+01 C288000200070
2.755 5.769E+01 C288000200071
2.804 6.046E+01 C288000200072
2.857 6.334E+01 C288000200073
2.911 6.814E+01 C288000200074
2.964 7.138E+01 C288000200075
3.002 7.296E+01 C288000200076
ENDDATA 62 0 C288000200077
ENDSUBENT 76 0 C288000299999
SUBENT C2880003 20230106 C226C288000300001
BIB 6 16 C288000300002
REACTION (4-BE-10(D,P)4-BE-11,,SIG) C288000300003
SAMPLE The target was 12+-1.6 keV thick at 3 MeV. C288000300004
METHOD From data recorded during two 11Be lifetimes C288000300005
(tau=19.6 sec) starting 6.6 sec after irradiation. C288000300006
Protons populating both the ground and 0.318-MeV C288000300007
states of 11Be contribute to the yield. C288000300008
RAD-DET (4-BE-11,B-) C288000300009
ERR-ANALYS (ERR-1) The uncertainty in the vertical scale is C288000300010
again about 43%, because of the same causes discussed C288000300011
in the (d,a) section. C288000300012
(ERR-2) In addition to the scale uncertainty, there C288000300013
may be a relative error of about 10% in the ratio of C288000300014
cross sections taken from extreme ends of the C288000300015
excitation function. C288000300016
STATUS (CURVE,,D.R.Goosman+,J,PR/C,1,1939,1970) C288000300017
Fig. 3, page 1940 of J,PR/C,1,1939,1970. C288000300018
ENDBIB 16 0 C288000300019
COMMON 2 3 C288000300020
ERR-1 ERR-2 C288000300021
PER-CENT PER-CENT C288000300022
43.0 10.0 C288000300023
ENDCOMMON 3 0 C288000300024
DATA 2 130 C288000300025
EN DATA C288000300026
MEV MB C288000300027
1.947 6.001E-01 C288000300028
1.963 7.027E-01 C288000300029
1.986 8.906E-01 C288000300030
2.029 9.876E-01 C288000300031
2.062 1.218E+00 C288000300032
2.116 1.350E+00 C288000300033
2.155 1.710E+00 C288000300034
2.193 1.847E+00 C288000300035
2.210 2.051E+00 C288000300036
2.248 2.275E+00 C288000300037
2.302 2.589E+00 C288000300038
2.345 2.872E+00 C288000300039
2.394 3.184E+00 C288000300040
2.432 3.626E+00 C288000300041
2.476 3.916E+00 C288000300042
2.524 4.228E+00 C288000300043
2.562 4.690E+00 C288000300044
2.616 4.676E+00 C288000300045
2.654 5.616E+00 C288000300046
2.692 6.067E+00 C288000300047
2.725 6.556E+00 C288000300048
2.774 6.894E+00 C288000300049
2.849 7.237E+00 C288000300050
2.914 7.603E+00 C288000300051
2.962 8.429E+00 C288000300052
3.033 9.583E+00 C288000300053
3.087 1.062E+01 C288000300054
3.136 1.117E+01 C288000300055
3.173 1.114E+01 C288000300056
3.233 1.302E+01 C288000300057
3.281 1.333E+01 C288000300058
3.325 1.402E+01 C288000300059
3.363 1.475E+01 C288000300060
3.427 1.470E+01 C288000300061
3.476 1.587E+01 C288000300062
3.535 1.712E+01 C288000300063
3.589 1.753E+01 C288000300064
3.638 1.843E+01 C288000300065
3.708 1.987E+01 C288000300066
3.762 2.034E+01 C288000300067
3.778 2.260E+01 C288000300068
3.837 2.136E+01 C288000300069
3.897 2.495E+01 C288000300070
3.962 2.621E+01 C288000300071
4.011 3.064E+01 C288000300072
4.059 3.488E+01 C288000300073
4.097 3.768E+01 C288000300074
4.162 4.285E+01 C288000300075
4.227 4.384E+01 C288000300076
4.308 5.115E+01 C288000300077
4.378 5.372E+01 C288000300078
4.459 5.789E+01 C288000300079
4.519 6.414E+01 C288000300080
4.573 6.566E+01 C288000300081
4.632 6.720E+01 C288000300082
4.686 7.063E+01 C288000300083
4.750 7.038E+01 C288000300084
4.820 7.391E+01 C288000300085
4.874 7.368E+01 C288000300086
4.922 7.156E+01 C288000300087
4.987 7.719E+01 C288000300088
5.068 8.102E+01 C288000300089
5.127 7.659E+01 C288000300090
5.197 7.235E+01 C288000300091
5.256 6.839E+01 C288000300092
5.309 7.001E+01 C288000300093
5.374 6.976E+01 C288000300094
5.438 6.592E+01 C288000300095
5.508 6.566E+01 C288000300096
5.562 6.546E+01 C288000300097
5.626 6.352E+01 C288000300098
5.685 6.500E+01 C288000300099
5.744 6.479E+01 C288000300100
5.798 6.126E+01 C288000300101
5.863 6.608E+01 C288000300102
5.922 6.414E+01 C288000300103
5.992 6.736E+01 C288000300104
6.020 5.472E+01 C288000300105
6.073 5.320E+01 C288000300106
6.143 5.305E+01 C288000300107
6.212 5.576E+01 C288000300108
6.289 5.276E+01 C288000300109
6.359 5.262E+01 C288000300110
6.436 5.385E+01 C288000300111
6.513 5.369E+01 C288000300112
6.574 5.218E+01 C288000300113
6.644 5.204E+01 C288000300114
6.721 5.189E+01 C288000300115
6.806 5.172E+01 C288000300116
6.883 5.156E+01 C288000300117
6.936 4.757E+01 C288000300118
7.014 4.869E+01 C288000300119
7.091 4.854E+01 C288000300120
7.183 4.712E+01 C288000300121
7.260 4.698E+01 C288000300122
7.330 4.810E+01 C288000300123
7.384 4.676E+01 C288000300124
7.453 4.787E+01 C288000300125
7.522 4.651E+01 C288000300126
7.592 4.519E+01 C288000300127
7.669 4.389E+01 C288000300128
7.738 4.493E+01 C288000300129
7.807 4.481E+01 C288000300130
7.884 4.240E+01 C288000300131
7.969 4.338E+01 C288000300132
8.015 4.331E+01 C288000300133
8.092 4.098E+01 C288000300134
8.154 4.307E+01 C288000300135
8.247 4.292E+01 C288000300136
8.331 4.060E+01 C288000300137
8.409 4.378E+01 C288000300138
8.486 4.253E+01 C288000300139
8.570 3.919E+01 C288000300140
8.624 4.121E+01 C288000300141
8.717 3.897E+01 C288000300142
8.801 3.884E+01 C288000300143
8.871 3.774E+01 C288000300144
8.963 3.760E+01 C288000300145
9.048 3.651E+01 C288000300146
9.140 3.277E+01 C288000300147
9.240 3.351E+01 C288000300148
9.302 3.522E+01 C288000300149
9.387 3.511E+01 C288000300150
9.487 3.590E+01 C288000300151
9.557 3.580E+01 C288000300152
9.618 3.666E+01 C288000300153
9.703 3.560E+01 C288000300154
9.804 3.640E+01 C288000300155
9.880 3.444E+01 C288000300156
9.973 3.432E+01 C288000300157
ENDDATA 132 0 C288000300158
ENDSUBENT 157 0 C288000399999
SUBENT C2880004 20230106 C226C288000400001
BIB 3 9 C288000400002
REACTION (4-BE-10(D,X)1-H-1,,DA/DE,,REL) C288000400003
METHOD The proton profiles taken with reflection geometry at C288000400004
153 and transmission geometry at 25 degrees. In both C288000400005
cases the acceptance angles in the theta and phi C288000400006
directions were 1 and 6 degrees, respectively, and C288000400007
the focal-plane aperture was set for an energy C288000400008
resolution of 0.28%. C288000400009
STATUS (CURVE,,D.R.Goosman+,J,PR/C,1,1939,1970) C288000400010
Fig. 4, page 1942 of J,PR/C,1,1939,1970. C288000400011
ENDBIB 9 0 C288000400012
COMMON 2 3 C288000400013
EN EN-RSL C288000400014
MEV PER-CENT C288000400015
6.0 0.28 C288000400016
ENDCOMMON 3 0 C288000400017
DATA 3 75 C288000400018
ANG E DATA C288000400019
ADEG MEV ARB-UNITS C288000400020
153.0 1.849 34.890E+00 C288000400021
153.0 1.860 29.950E+00 C288000400022
153.0 1.875 33.070E+00 C288000400023
153.0 1.893 44.680E+00 C288000400024
153.0 1.902 83.230E+00 C288000400025
153.0 1.912 69.070E+00 C288000400026
153.0 1.924 37.620E+00 C288000400027
153.0 1.935 45.220E+00 C288000400028
153.0 1.937 55.330E+00 C288000400029
153.0 1.950 48.280E+00 C288000400030
153.0 1.961 58.030E+00 C288000400031
153.0 1.972 81.160E+00 C288000400032
153.0 1.984141.300E+00 C288000400033
153.0 2.006541.900E+00 C288000400034
153.0 2.026 1.153E+03 C288000400035
153.0 2.031 1.078E+03 C288000400036
153.0 2.038244.700E+00 C288000400037
153.0 2.058118.300E+00 C288000400038
153.0 2.071103.300E+00 C288000400039
153.0 2.079162.600E+00 C288000400040
153.0 2.090247.300E+00 C288000400041
153.0 2.097151.600E+00 C288000400042
153.0 2.103 89.900E+00 C288000400043
153.0 2.110 44.290E+00 C288000400044
153.0 2.122 36.750E+00 C288000400045
153.0 2.129 27.580E+00 C288000400046
153.0 2.144 47.180E+00 C288000400047
153.0 2.151 97.250E+00 C288000400048
153.0 2.159 55.740E+00 C288000400049
153.0 2.165 27.000E+00 C288000400050
153.0 2.183 17.990E+00 C288000400051
153.0 2.197 20.200E+00 C288000400052
153.0 2.212 25.530E+00 C288000400053
153.0 2.221 45.980E+00 C288000400054
153.0 2.227 93.190E+00 C288000400055
153.0 2.242445.300E+00 C288000400056
153.0 2.248 3.906E+03 C288000400057
153.0 2.248 1.831E+03 C288000400058
153.0 2.249 2.607E+03 C288000400059
153.0 2.261 4.854E+03 C288000400060
153.0 2.271146.100E+00 C288000400061
153.0 2.272482.700E+00 C288000400062
153.0 2.278 70.750E+00 C288000400063
153.0 2.285 8.330E+00 C288000400064
25.0 3.301 64.540E+00 C288000400065
25.0 3.326 45.860E+00 C288000400066
25.0 3.341 73.360E+00 C288000400067
25.0 3.365 76.850E+00 C288000400068
25.0 3.380 92.290E+00 C288000400069
25.0 3.404174.500E+00 C288000400070
25.0 3.423324.600E+00 C288000400071
25.0 3.440370.400E+00 C288000400072
25.0 3.465316.900E+00 C288000400073
25.0 3.497 87.460E+00 C288000400074
25.0 3.541 34.330E+00 C288000400075
25.0 3.559 47.150E+00 C288000400076
25.0 3.581 42.450E+00 C288000400077
25.0 3.598 50.960E+00 C288000400078
25.0 3.617135.100E+00 C288000400079
25.0 3.646423.300E+00 C288000400080
25.0 3.664 1.049E+03 C288000400081
25.0 3.679 1.796E+03 C288000400082
25.0 3.687 2.196E+03 C288000400083
25.0 3.698 1.790E+03 C288000400084
25.0 3.722 1.039E+03 C288000400085
25.0 3.739 1.427E+03 C288000400086
25.0 3.777 5.467E+03 C288000400087
25.0 3.801 7.630E+03 C288000400088
25.0 3.811 8.866E+03 C288000400089
25.0 3.821 7.604E+03 C288000400090
25.0 3.840 4.493E+03 C288000400091
25.0 3.862 1.470E+03 C288000400092
25.0 3.882721.500E+00 C288000400093
25.0 3.901360.100E+00 C288000400094
25.0 3.918216.500E+00 C288000400095
ENDDATA 77 0 C288000400096
ENDSUBENT 95 0 C288000499999
SUBENT C2880005 20230106 C226C288000500001
BIB 5 14 C288000500002
REACTION (4-BE-10(D,P)4-BE-11,PAR,DA) C288000500003
METHOD Protons populating the 0.318-MeV level in 11Be were C288000500004
well resolved, however, and their angular C288000500005
distribution was measured in the forward hemisphere, C288000500006
using the 10Be target on the thin Pt backing. C288000500007
CORRECTION At each angle, the protons were scanned over a C288000500008
200-keV energy range, substantially greater than the C288000500009
35-keV width of the proton group, in order to C288000500010
determine the small continuum background underlying C288000500011
the peak. C288000500012
ERR-ANALYS (DATA-ERR) The error bars reflect the uncertainty in C288000500013
this correction as well as counting statistics. C288000500014
STATUS (CURVE,,D.R.Goosman+,J,PR/C,1,1939,1970) C288000500015
Fig. 5, page 1942 of J,PR/C,1,1939,1970. C288000500016
ENDBIB 14 0 C288000500017
COMMON 2 3 C288000500018
EN E-LVL C288000500019
MEV MEV C288000500020
6.0 0.318 C288000500021
ENDCOMMON 3 0 C288000500022
DATA 3 7 C288000500023
ANG-CM DATA-CM DATA-ERR C288000500024
ADEG MB/SR MB/SR C288000500025
6.203 26.611 1.369 C288000500026
11.872 22.583 1.364 C288000500027
17.924 18.420 1.559 C288000500028
23.654 12.379 1.300 C288000500029
35.159 5.424 0.973 C288000500030
46.509 1.457 0.388 C288000500031
57.849 0.997 0.519 C288000500032
ENDDATA 9 0 C288000500033
ENDSUBENT 32 0 C288000599999
ENDENTRY 5 0 C288099999999