ENTRY C2880 20230106 C288000000001 SUBENT C2880001 20230106 20231011 C288000100001 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 20231011 C288000200001 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 20231011 C288000300001 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 20231011 C288000400001 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 20231011 C288000500001 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