ENTRY C0982 20161216 C164C098200000001 SUBENT C0982001 20161216 C164C098200100001 BIB 11 35 C098200100002 TITLE Experimental Study of Level Density and C098200100003 gamma-strength Functions from Compound Nuclear C098200100004 Reactions C098200100005 AUTHOR (A.V.Voinov,S.M.Grimes,C.R.Brune,M.Guttormsen, C098200100006 T.N.Massey, A.Schiller,S.Siem) C098200100007 REFERENCE (S,AIP-1005,61,2008) C098200100008 #doi:10.1063/1.2920747 C098200100009 REL-REF (I,,A.V.Voinov+,J,PR/C,76,044602,2007) Charged particleC098200100010 and neutron spectrometer descriptions. C098200100011 (O,C2087001,A.P.D.Ramirez+,J,PR/C,88,064324,2013) C098200100012 65Cu(d,n) cross sections. C098200100013 (O,C1685001,A.V.Voinov+,J,PR/C,79,031301,2009) C098200100014 59Co(d,n) cross sections. C098200100015 (O,C1783001,A.V.Voinov+,J,PR/C,81,024319,2010) C098200100016 59Co(p,g) cross sections. C098200100017 INSTITUTE (1USAOHO,2NOROSL) C098200100018 FACILITY (VDGT,1USAOHO) The tandem accelerator at Ohio C098200100019 University's Edwards Accelerator Laboratory. C098200100020 DETECTOR (SCIN,SPEC) NE213 Liquid scintillators. Charged C098200100021 particle spectrometer. C098200100022 PART-DET (N) C098200100023 METHOD (TOF) The outgoing charged particles were registered C098200100024 by a charged-particle spectrometer allowing the C098200100025 measurement of both energy and angular distributions C098200100026 of outgoing particles. Particle masses are determined C098200100027 by measuring both the energy deposited in Si C098200100028 detectors and the time of flight with a 2 m flight C098200100029 path. Neutrons are registered by liquid scintillators C098200100030 set up at the distance of about 7 m from the target. C098200100031 The pulsed beam and time of flight technique are used C098200100032 to determine the energies of outgoing neutrons. The C098200100033 particles are mostly registered at backward angles to C098200100034 reduce direct reaction contributions. C098200100035 STATUS (APRVD) Approved by A. Voinov on January 13, 2017. C098200100036 HISTORY (20161216C) BP C098200100037 ENDBIB 35 0 C098200100038 NOCOMMON 0 0 C098200100039 ENDSUBENT 38 0 C098200199999 SUBENT C0982002 20161216 C164C098200200001 BIB 5 8 C098200200002 REACTION (13-AL-27(D,X)0-NN-1,,DA/DE) C098200200003 COMMENT Cross sections include all neutrons, mostly from C098200200004 (d,n)+(d,pn) channels. C098200200005 ERR-ANALYS (ERR-S) Statistical errors only. C098200200006 STATUS (TABLE) Data were received from A. Voinov. C098200200007 These data were used to produce level C098200200008 densities shown in Fig.1 page 62. C098200200009 HISTORY (20170113R) Data received from Voinov C098200200010 ENDBIB 8 0 C098200200011 COMMON 2 3 C098200200012 EN ANG C098200200013 MEV ADEG C098200200014 7.5 120.0 C098200200015 ENDCOMMON 3 0 C098200200016 DATA 3 49 C098200200017 E DATA-CM ERR-S C098200200018 MEV MB/SR/MEV MB/SR/MEV C098200200019 1.05000E+0 2.99984E+0 1.39983E-1 C098200200020 1.35000E+0 7.49702E+0 3.36886E-1 C098200200021 1.65000E+0 1.00732E+1 4.40446E-1 C098200200022 1.95000E+0 1.07642E+1 4.76335E-1 C098200200023 2.25000E+0 9.74737E+0 4.44857E-1 C098200200024 2.55000E+0 7.77063E+0 3.69004E-1 C098200200025 2.85000E+0 6.21988E+0 3.07619E-1 C098200200026 3.15000E+0 6.28003E+0 3.22141E-1 C098200200027 3.45000E+0 5.10678E+0 2.71275E-1 C098200200028 3.75000E+0 3.89607E+0 2.14032E-1 C098200200029 4.05000E+0 4.09808E+0 2.31701E-1 C098200200030 4.35000E+0 3.22267E+0 1.87429E-1 C098200200031 4.65000E+0 3.92085E+0 2.33198E-1 C098200200032 4.95000E+0 2.55990E+0 1.56341E-1 C098200200033 5.25000E+0 2.30544E+0 1.43479E-1 C098200200034 5.55000E+0 2.20276E+0 1.39368E-1 C098200200035 5.85000E+0 1.91805E+0 1.23389E-1 C098200200036 6.15000E+0 1.23539E+0 8.13623E-2 C098200200037 6.45000E+0 1.72308E+0 1.14420E-1 C098200200038 6.75000E+0 1.44802E+0 9.77142E-2 C098200200039 7.05000E+0 9.59761E-1 6.66886E-2 C098200200040 7.35000E+0 1.01597E+0 7.20635E-2 C098200200041 7.65000E+0 1.15725E+0 8.42078E-2 C098200200042 7.95000E+0 8.91688E-1 6.79182E-2 C098200200043 8.25000E+0 5.93008E-1 4.74642E-2 C098200200044 8.55000E+0 5.83422E-1 4.88822E-2 C098200200045 8.85000E+0 8.56162E-1 7.40467E-2 C098200200046 9.15000E+0 9.50932E-1 8.56521E-2 C098200200047 9.45000E+0 7.65869E-1 7.28015E-2 C098200200048 9.75000E+0 4.51751E-1 4.54573E-2 C098200200049 1.00500E+1 1.57697E-1 1.75100E-2 C098200200050 1.03500E+1 4.63259E-2 6.53003E-3 C098200200051 1.06500E+1 1.08618E-1 1.36154E-2 C098200200052 1.09500E+1 2.71734E-1 3.36587E-2 C098200200053 1.12500E+1 3.53268E-1 4.50808E-2 C098200200054 1.15500E+1 2.00162E-1 2.69128E-2 C098200200055 1.18500E+1 3.64654E-2 6.01493E-3 C098200200056 1.21500E+1 1.44146E-2 2.88292E-3 C098200200057 1.24500E+1 1.12375E-2 2.44363E-3 C098200200058 1.27500E+1 1.63667E-2 3.32986E-3 C098200200059 1.30500E+1 3.27411E-2 5.77784E-3 C098200200060 1.33500E+1 6.24638E-2 1.11865E-2 C098200200061 1.36500E+1 2.06330E-1 4.04269E-2 C098200200062 1.39500E+1 4.18618E-1 9.34387E-2 C098200200063 1.42500E+1 3.20775E-1 9.05446E-2 C098200200064 1.45500E+1 6.71331E-2 3.47461E-2 C098200200065 1.48500E+1 1.31465E-2 2.32460E-2 C098200200066 1.51500E+1 3.30216E-3 6.25979E-2 C098200200067 1.54500E+1 6.35884E-4 1.27177E-1 C098200200068 ENDDATA 51 0 C098200200069 ENDSUBENT 68 0 C098200299999 ENDENTRY 2 0 C098299999999