ENTRY C2161 20150527 C151C216100000001 SUBENT C2161001 20150527 C151C216100100001 BIB 11 23 C216100100002 TITLE Single particle strengths and mirror states in 15N - C216100100003 15-O below 12.0 MeV C216100100004 AUTHOR (C.E.Mertin,D.D.Caussyn,A.M.Crisp,N.Keeley,K.W.Kemper, C216100100005 O.Momotyuk,B.T.Roeder,A.Volya) C216100100006 INSTITUTE (1USAFSU,3POLIPJ) C216100100007 REFERENCE (J,PR/C,91,044317,2015) C216100100008 REL-REF (C,A1450008,J.P.Schiffer+,J,PR,164,1274,1967) Data C216100100009 shown in fig. 4a of the reference are not compiled C216100100010 in C2161 because they are taken from REL-REF. C216100100011 FACILITY (VDGT,1USAFSU) C216100100012 (LINAC,1USAFSU) Experiment performed using Florida C216100100013 State University tandem-linac accelerator combination. C216100100014 SAMPLE Target was natural melamine (C3H6N6) target with C216100100015 thickness of about 300 mu-g/cm2 on a 20 mu-g/cm2 C216100100016 carbon backing C216100100017 DETECTOR (TELES,SI,SI) A dE-E silicon detector telescope was C216100100018 used to measure the outgoing protons and deuterons. A C216100100019 single silicon detector on the opposite side of the C216100100020 incoming beam served as a monitor of the target C216100100021 conditions. C216100100022 METHOD (EDE) C216100100023 ERR-ANALYS (DATA-ERR) No information given C216100100024 HISTORY (20150527C) Compiled by S.H. C216100100025 ENDBIB 23 0 C216100100026 COMMON 1 3 C216100100027 EN C216100100028 MEV C216100100029 16.0 C216100100030 ENDCOMMON 3 0 C216100100031 ENDSUBENT 30 0 C216100199999 SUBENT C2161002 20150527 C151C216100200001 BIB 5 19 C216100200002 REACTION (7-N-14(D,P)7-N-15,PAR,DA) C216100200003 STATUS (TABLE) Data presented in fig. 3,4 and 5 of the C216100200004 reference, sent by author (C.E.M.) C216100200005 EN-SEC (E-LVL,7-N-15) C216100200006 MONITOR (7-N-14(D,EL)7-N-14,PAR,DA) C216100200007 (6-C-12(D,EL)6-C-12,PAR,DA) C216100200008 Absolute cross section of 14N(d,p) reaction was C216100200009 determined using previously measured deuteron elastic C216100200010 scattering cross section on 12C and 14N C216100200011 METHOD To determine the contribution of carbon to elastic C216100200012 scattering with melamine target, ratio of the yield C216100200013 for the 4.4 MeV first excited state in 12C to that for C216100200014 the 12C ground state for the deuteron scattering by C216100200015 the carbon target was measured at at all angles. The C216100200016 elastic nitrogen yield was determined by extracting C216100200017 the 4.4 MeV yield from the melamine target and C216100200018 using the yield ratio from the carbon target to C216100200019 subtract its contribution to the total nitrogen C216100200020 plus carbon elastic yield. C216100200021 ENDBIB 19 0 C216100200022 NOCOMMON 0 0 C216100200023 DATA 5 64 C216100200024 E-LVL E-LVL ANG-CM DATA-CM DATA-ERR C216100200025 MEV MEV ADEG MB/SR MB/SR C216100200026 5.270 5.299 10.88 0.981 0.182 C216100200027 5.270 5.299 16.31 1.058 0.169 C216100200028 5.270 5.299 21.73 0.824 0.126 C216100200029 5.270 5.299 27.14 0.539 0.092 C216100200030 5.270 5.299 32.53 0.493 0.073 C216100200031 5.270 5.299 37.90 0.431 0.072 C216100200032 6.323 10.91 2.300 0.279 C216100200033 6.323 16.35 1.845 0.224 C216100200034 6.323 21.79 1.226 0.153 C216100200035 6.323 27.21 0.602 0.098 C216100200036 6.323 32.61 0.375 0.063 C216100200037 6.323 38.00 0.299 0.060 C216100200038 7.155 10.93 14.305 0.696 C216100200039 7.155 16.39 12.127 0.574 C216100200040 7.155 21.83 10.137 0.441 C216100200041 7.155 27.27 7.736 0.350 C216100200042 7.155 32.68 4.830 0.227 C216100200043 7.155 38.08 3.052 0.191 C216100200044 7.300 10.94 28.103 0.975 C216100200045 7.300 16.39 8.031 0.467 C216100200046 7.300 21.84 2.261 0.208 C216100200047 7.300 27.28 4.534 0.268 C216100200048 7.300 32.69 5.912 0.252 C216100200049 7.300 38.09 5.242 0.250 C216100200050 7.567 10.94 17.112 0.761 C216100200051 7.567 16.41 16.278 0.665 C216100200052 7.567 21.86 13.050 0.500 C216100200053 7.567 27.30 10.194 0.402 C216100200054 7.567 32.72 6.587 0.266 C216100200055 7.567 38.12 3.865 0.215 C216100200056 8.312 10.97 12.953 0.662 C216100200057 8.312 16.44 2.713 0.271 C216100200058 8.312 21.91 1.054 0.142 C216100200059 8.312 27.36 2.378 0.194 C216100200060 8.312 32.79 2.806 0.173 C216100200061 8.312 38.20 2.681 0.179 C216100200062 8.571 10.98 2.705 0.302 C216100200063 8.571 16.46 1.357 0.192 C216100200064 8.571 27.38 1.458 0.152 C216100200065 8.571 32.81 0.910 0.099 C216100200066 8.571 38.23 0.467 0.075 C216100200067 10.066 11.03 16.165 0.739 C216100200068 10.066 16.54 10.852 0.543 C216100200069 10.066 22.04 7.742 0.385 C216100200070 10.066 27.52 6.119 0.311 C216100200071 10.066 32.98 3.898 0.204 C216100200072 10.066 38.41 2.214 0.163 C216100200073 11.236 11.09 10.925 0.638 C216100200074 11.236 16.62 7.469 0.479 C216100200075 11.236 22.14 5.054 0.322 C216100200076 11.236 27.64 3.435 0.244 C216100200077 11.236 33.13 2.023 0.151 C216100200078 11.236 38.59 1.341 0.133 C216100200079 12.145 11.13 20.156 0.826 C216100200080 12.145 16.69 13.592 0.607 C216100200081 12.145 22.23 5.136 0.314 C216100200082 12.145 33.26 1.596 0.131 C216100200083 12.145 38.74 1.496 0.134 C216100200084 12.493 11.15 11.397 0.621 C216100200085 12.493 16.72 7.868 0.462 C216100200086 12.493 22.27 5.787 0.333 C216100200087 12.493 27.80 3.408 0.232 C216100200088 12.493 33.31 1.639 0.132 C216100200089 12.493 38.80 1.029 0.111 C216100200090 ENDDATA 66 0 C216100200091 ENDSUBENT 90 0 C216100299999 ENDENTRY 2 0 C216199999999