ENTRY C2204 20160922 C165C220400000001 SUBENT C2204001 20160922 C165C220400100001 BIB 11 40 C220400100002 TITLE Population of 13Be in a nucleon exchange reaction C220400100003 AUTHOR (B.R.Marks,P.A.DeYoung,J.K.Smith,T.Baumann,J.Brown, C220400100004 N.Frank,J.Hinnefeld,M.Hoffman,M.D.Jones,Z.Kohley, C220400100005 A.N.Kuchera,B.Luther,A.Spyrou,S.Stephenson,C.Sullivan, C220400100006 M.Thoennessen,N.Viscariello,S.J.Williams) C220400100007 INSTITUTE (1USAHPE,1USAMSU,1USAISB) C220400100008 (1USAUSA) Wabash College, Crawfordsville, Indiana C220400100009 (1USAUSA) Augustana College, Rock Island, Illinois C220400100010 (1USAUSA) Concordia College, Moorhead, Minnesota C220400100011 (1USAUSA) Gettysburg College, Gettysburg, Pennsylvania C220400100012 REFERENCE (J,PR/C,92,054320,2015) C220400100013 FACILITY (CYCTM,1USAMSU) The experiment was performed at the C220400100014 National Superconducting Cyclotron Laboratory at C220400100015 Michigan State University using Coupled Cyclotron C220400100016 Facility C220400100017 SAMPLE 9Be target with thickness of 51 mg/cm2 C220400100018 DETECTOR (MAGSP) The 12Be reaction products were deflected by C220400100019 a large-gap sweeper magnet and identified from C220400100020 energy-loss and time-of-flight measurements. C220400100021 (SCIN) Neutrons were detected using MoNA array. The C220400100022 MoNA consists of 144 individual detector modules. Each C220400100023 module is based on a 200 x 10 x 10 cm3 block of BC-408 C220400100024 plastic scintillator. In the nominal configuration the C220400100025 vertical layers of 16 of the scintillator blocks give C220400100026 a detector volume of 2.0 x 1.6 x 0.9 m3. Neutron energyC220400100027 and position was determined from time of flight. C220400100028 METHOD (COINC) Coincidence between charged particle reaction C220400100029 products and neutrons were required. C220400100030 (TOF) Momentum and energy of neutrons were determined C220400100031 from time of flight measurement C220400100032 INC-SOURCE Primary beam 18-O with energy of 120MeV/A bombarded a C220400100033 2.5 g/cm2 9Be production target. The A1900 fragment C220400100034 separator was used to separate and select the 13B C220400100035 secondary beam. The final energy of the beam was 71 C220400100036 MeV/A, with an intensity of approximately 8.0E+5 C220400100037 particles per second and a purity of 96%. 13Be was C220400100038 produced in a nucleon exchange reaction and immediatelyC220400100039 decayed into 12Be + n. C220400100040 ERR-ANALYS (DATA-ERR) Source of uncertainties unknown C220400100041 HISTORY (20160922C) Compiled by S.H. C220400100042 ENDBIB 40 0 C220400100043 NOCOMMON 0 0 C220400100044 ENDSUBENT 43 0 C220400199999 SUBENT C2204002 20160922 C165C220400200001 BIB 2 2 C220400200002 REACTION (5-B-13(4-BE-9,X)4-BE-13,,SIG) C220400200003 STATUS (TABLE) Data taken from text p. 2 of the reference C220400200004 ENDBIB 2 0 C220400200005 NOCOMMON 0 0 C220400200006 DATA 3 1 C220400200007 EN DATA DATA-ERR C220400200008 MEV/A MB MB C220400200009 71.0 0.30 0.15 C220400200010 ENDDATA 3 0 C220400200011 ENDSUBENT 10 0 C220400299999 SUBENT C2204003 20160922 C165C220400300001 BIB 3 7 C220400300002 REACTION 1(5-B-13(N,0),,EN) C220400300003 2(5-B-13(N,P),,WID) C220400300004 3(5-B-13(N,P),,J) C220400300005 4(5-B-13(N,P),,PTY) C220400300006 STATUS (TABLE) Data taken from tab. 1 of the reference C220400300007 ANALYSIS Data obtained by analysis of decay energy C220400300008 spectrum of 13Be. C220400300009 ENDBIB 7 0 C220400300010 NOCOMMON 0 0 C220400300011 DATA 6 2 C220400300012 DATA 1DATA-ERR 1DATA 2DATA-ERR 2DATA 3DATA 4C220400300013 MEV MEV MEV MEV NO-DIM NO-DIM C220400300014 1.05 0.1 0.5 0.2 2.5 +1. C220400300015 2.56 0.13 2.29 0.73 2.5 +1. C220400300016 ENDDATA 4 0 C220400300017 ENDSUBENT 16 0 C220400399999 ENDENTRY 3 0 C220499999999