ENTRY C1953 20121102 C124C195300000001 SUBENT C1953001 20121102 C124C195300100001 BIB 10 40 C195300100002 TITLE Neutron Single Particle Structure in 131Sn and Direct C195300100003 Neutron Capture Cross Sections C195300100004 AUTHOR (R.L.Kozub,G.Arbanas,A.S.Adekola,D.W.Bardayan, C195300100005 J.C.Blackmon,K.Y.Chae,K.A.Chipps,J.A.Cizewski, C195300100006 L.Erikson,R.Hatarik,W.R.Hix,K.L.Jones,W.Krolas, C195300100007 J.F.Liang,Z.Ma,C.Matei,B.H.Moazen,C.D.Nesaraja, C195300100008 S.D.Pain,D.Shapira,J.F.Shriner Jr,M.S.Smith,T.P.Swan) C195300100009 INSTITUTE (1USATTU,1USAORL,1USAOHO,1USARUT,1USATEN,1USACSM, C195300100010 3POLIFJ,1USAOAU,2UK SUR) C195300100011 (3KORKOR) Sungkyunkwan University, Suwon C195300100012 REFERENCE (J,PRL,109,172501,2012) C195300100013 FACILITY (VDGT,1USAORL) Experiment performed at the Holifield C195300100014 Radioactive Ion Beam Facility at Oak Ridge National C195300100015 Laboratory C195300100016 SAMPLE Polyethylene foil (CD2)n with thickness of 80 mu-g/cm2 C195300100017 The target surface was placed at 30deg with respect to C195300100018 the beam axis, so the effective areal density was C195300100019 160 mu-g/cm2. Inverse kinematics was used. C195300100020 DETECTOR (TELES,SI,SISD) The ORRUBA array consisted of ten C195300100021 1000 mu-m thick position sensitive silicon strip C195300100022 detectors, plus four thinner dE detectors that were C195300100023 used to form detector telescopes for the more forward C195300100024 angles C195300100025 (SISD,MCPLT) Annular silicon strip detector, a carbon- C195300100026 foil-microchannel plate detector, and a C195300100027 segmented-anode ion counter were placed at forward C195300100028 angle and used for beam diagnostic. C195300100029 METHOD (EDE) E-dE method was used for particle identification.C195300100030 (COINC) Coincidence signals from particles detected C195300100031 in the ORRUBA silicon arrays and the beamlike recoils C195300100032 striking the microchannel plate detector served to C195300100033 reduce the background from other, non-(d,p) processes C195300100034 Inverse kinematics was used C195300100035 ANALYSIS Cross section normalization was achieved by detecting C195300100036 elastically scattered deuterons with the ORRUBA at C195300100037 relatively small center-of-mass angles C195300100038 33deg-38deg, where the ratio to Rutherford C195300100039 scattering is in the range 0.92 - 0.99, and comparing C195300100040 to optical model calculations. C195300100041 HISTORY (20121102C)Compiled by S.H. C195300100042 ENDBIB 40 0 C195300100043 NOCOMMON 0 0 C195300100044 ENDSUBENT 43 0 C195300199999 SUBENT C1953002 20121102 C124C195300200001 BIB 4 8 C195300200002 REACTION ((1-H-2(50-SN-130,P)50-SN-131,PAR,DA,RSD)= C195300200003 (50-SN-130(D,P)50-SN-131,PAR,DA)) C195300200004 STATUS (TABLE) Data presented in fig 3 of the reference C195300200005 sent by author (R.L.K.) C195300200006 ERR-ANALYS (ERR-S) Statistical uncertainty C195300200007 (ERR-SYS) Systematic uncertainty in cross section C195300200008 normalization C195300200009 EN-SEC (E-LVL,50-SN-131) C195300200010 ENDBIB 8 0 C195300200011 COMMON 2 3 C195300200012 EN ERR-SYS C195300200013 MEV/A PER-CENT C195300200014 4.8 10.0 C195300200015 ENDCOMMON 3 0 C195300200016 DATA 4 32 C195300200017 E-LVL ANG-CM DATA-CM ERR-S C195300200018 KEV ADEG MB/SR MB/SR C195300200019 2628.0 24.4 2.0 0.6 C195300200020 2628.0 27.5 3.1 0.6 C195300200021 2628.0 31.0 3.3 0.6 C195300200022 2628.0 34.7 4.9 0.6 C195300200023 2628.0 38.9 4.7 0.5 C195300200024 2628.0 43.4 5.1 1.0 C195300200025 2628.0 48.4 3.9 0.8 C195300200026 2628.0 53.8 3.0 0.7 C195300200027 2628.0 59.6 4.2 0.7 C195300200028 2628.0 65.8 2.1 0.5 C195300200029 3404.0 22.6 11.5 1.3 C195300200030 3404.0 25.6 7.6 1.0 C195300200031 3404.0 28.9 7.0 0.8 C195300200032 3404.0 32.6 9.4 0.8 C195300200033 3404.0 36.7 7.8 0.7 C195300200034 3404.0 41.2 9.4 1.3 C195300200035 3404.0 46.2 11.1 1.3 C195300200036 3404.0 51.6 9.5 1.1 C195300200037 3404.0 57.4 9.5 1.0 C195300200038 3404.0 63.7 9.3 0.9 C195300200039 3986.0 27.0 7.0 0.9 C195300200040 3986.0 30.6 6.0 0.7 C195300200041 3986.0 34.6 5.3 0.6 C195300200042 3986.0 44.1 6.4 1.0 C195300200043 3986.0 49.5 6.8 0.9 C195300200044 3986.0 55.4 7.8 0.9 C195300200045 3986.0 61.8 7.2 0.9 C195300200046 4655.0 28.0 5.5 0.7 C195300200047 4655.0 32.0 4.6 0.6 C195300200048 4655.0 46.9 5.5 0.9 C195300200049 4655.0 52.9 5.9 0.8 C195300200050 4655.0 59.4 5.1 0.8 C195300200051 ENDDATA 34 0 C195300200052 ENDSUBENT 51 0 C195300299999 ENDENTRY 2 0 C195399999999