ENTRY L0209 20151106 L028L020900000001 SUBENT L0209001 20151106 L028L020900100001 BIB 12 29 L020900100002 TITLE Photodisintegration of 7Li with progeny nuclei in L020900100003 excited states L020900100004 AUTHOR (W.A.Wurtz,R.E.Pywell,B.E.Norum,S.Kucuker,B.D.Sawatzky,L020900100005 H.R.Weller,S.Stave,M.W.Ahmed) L020900100006 INSTITUTE (1CANSAS,1USAVIR,1USACBF,1USATNL,1USANCC) L020900100007 REFERENCE (J,PR/C,92,044603,2015) L020900100008 FACILITY (ESTRG,1USATNL) Experiment performed at the High L020900100009 Intensity gamma-ray Source (HIgS) at Triangle L020900100010 Universities Nuclear Laboratory, Durham L020900100011 SAMPLE Natural Li target L020900100012 DETECTOR (SCIN) Neutrons were detected using the Blowfish L020900100013 Neutron Detector Array. Blowfish is a segmented L020900100014 fast-neutron detector using 88 neutron detecting L020900100015 cells filled with BC-505 liquid scintillator. The L020900100016 cells are arranged in a sphere with the front face of L020900100017 each cell at a radius of 40.6 cm from the center. L020900100018 Blowfish has an angular acceptance of approximately L020900100019 1/4 of 4Pi. L020900100020 METHOD (TOF,PSD) Using Blowfish it is possible to measure L020900100021 for each event the light-output, time-of-flight for L020900100022 neutron energy determination and pulse-shape L020900100023 discrimination spectra for neutron identification. L020900100024 INC-SOURCE (LCS) At HIgS nearly monoenergetic gamma-rays were L020900100025 produced by Compton backscattering of photons on L020900100026 relativistic electrons in electron storage ring L020900100027 ERR-ANALYS (DATA-ERR) No information given L020900100028 HISTORY (20151106C) Compiled by S.H. L020900100029 CORRECTION Corrections for neutron scattering and finite geometry L020900100030 were calculated with the help of GEANT4 simulations L020900100031 ENDBIB 29 0 L020900100032 NOCOMMON 0 0 L020900100033 ENDSUBENT 32 0 L020900199999 SUBENT L0209002 20151106 L028L020900200001 BIB 2 2 L020900200002 REACTION (3-LI-7(G,N)3-LI-6,PAR,SIG) L020900200003 STATUS (TABLE) data taken from tab. 3 of the reference L020900200004 ENDBIB 2 0 L020900200005 COMMON 1 3 L020900200006 E-LVL L020900200007 MEV L020900200008 2.19 L020900200009 ENDCOMMON 3 0 L020900200010 DATA 3 2 L020900200011 EN DATA DATA-ERR L020900200012 MEV MB MB L020900200013 13.0 0.080 0.003 L020900200014 15.0 0.323 0.009 L020900200015 ENDDATA 4 0 L020900200016 ENDSUBENT 15 0 L020900299999 SUBENT L0209003 20151106 L028L020900300001 BIB 2 2 L020900300002 REACTION (3-LI-7(G,N)3-LI-6,PAR,SIG) L020900300003 STATUS (TABLE) data taken from tab. 3 of the reference L020900300004 ENDBIB 2 0 L020900300005 COMMON 1 3 L020900300006 E-LVL L020900300007 MEV L020900300008 3.56 L020900300009 ENDCOMMON 3 0 L020900300010 DATA 3 1 L020900300011 EN DATA DATA-ERR L020900300012 MEV MB MB L020900300013 15.0 0.124 0.004 L020900300014 ENDDATA 3 0 L020900300015 ENDSUBENT 14 0 L020900399999 SUBENT L0209004 20151106 L028L020900400001 BIB 3 3 L020900400002 REACTION (3-LI-7(G,D)2-HE-5,PAR,SIG) L020900400003 PART-DET (N) Neutrons from 5He->n+a L020900400004 STATUS (TABLE) data taken from tab. 3 of the reference L020900400005 ENDBIB 3 0 L020900400006 COMMON 1 3 L020900400007 E-LVL L020900400008 MEV L020900400009 1.27 L020900400010 ENDCOMMON 3 0 L020900400011 DATA 3 3 L020900400012 EN DATA-MAX DATA-ERR L020900400013 MEV MB MB L020900400014 12.0 0.20 0.01 L020900400015 13.0 0.28 0.01 L020900400016 15.0 0.25 0.01 L020900400017 ENDDATA 5 0 L020900400018 ENDSUBENT 17 0 L020900499999 ENDENTRY 4 0 L020999999999