ENTRY C2210 20160224 C157C221000000001 SUBENT C2210001 20160224 C157C221000100001 BIB 10 41 C221000100002 TITLE Structure of 107Sn studied through single-neutron C221000100003 knockout reactions C221000100004 AUTHOR (G.Cerizza,A.Ayres,K.L.Jones,R.Grzywacz,A.Bey, C221000100005 C.Bingham,L.Cartegni,D.Miller,S.Padgett,T.Baugher, C221000100006 D.Bazin,J.S.Berryman,A.Gade,S.McDaniel,A.Ratkiewicz, C221000100007 A.Shore,S.R.Stroberg, D.Weisshaar,K.Wimmer,R.Winkler, C221000100008 S.D.Pain,K.Y.Chae,J.A.Cizewski,M.E.Howard,J.A.Tostevin)C221000100009 INSTITUTE (1USATEN,1USAMSU,1USAORL,1USARUT,2UK SUR) C221000100010 REFERENCE (J,PR/C,93,021601,2016) C221000100011 FACILITY (CYCTM,1USAMSU) Experiment performed using coupled C221000100012 cyclotrons of the National Superconducting Cyclotron C221000100013 Laboratory at Michigan State University. C221000100014 SAMPLE The secondary tin beams impinged on a 47 mg/cm2 9Be C221000100015 reaction target at the target position of the S800 C221000100016 magnetic spectrometer C221000100017 DETECTOR (MAGSP) The reaction residues were momentum analysed C221000100018 using S800 magnetic spectrometer. C221000100019 (DRFTC) Two cathode readout drift chambers measured C221000100020 the particle positions and angles in the focal plane. C221000100021 These were used to reconstruct momentum distributions C221000100022 of the reaction residues. C221000100023 (CSICR) The secondary target was surrounded by the C221000100024 high-efficiency CsI(Na) scintillator array (CAESAR) C221000100025 that was used to identify the decay gamma rays of the C221000100026 reaction products. CAESAR consists of 192 CsI(Na) C221000100027 crystals with 95% of solid-angle coverage. The C221000100028 granularity of the array enables event-by-event C221000100029 Doppler reconstruction of gamma rays emitted in-flight.C221000100030 (SCIN,IOCH) The reaction residues were identified C221000100031 event by event by using the time of flight between C221000100032 two plastic scintillators and the energy loss dE C221000100033 measured in the S800 focal-plane ion chamber. C221000100034 METHOD (COINC,EDE,TOF) Particle energy determination for EdE C221000100035 method was made using time of flight C221000100036 INC-SOURCE Primary 124Xe beam was accelerated to 140 MeV/A. Two C221000100037 settings of the A1900 fragment separator were used to C221000100038 select 108Sn and 106Sn secondary beams and to deliver C221000100039 them to the target position of the S800 spectrograph. C221000100040 The average rate of 108Sn on the reaction target C221000100041 was 3000 pps. C221000100042 HISTORY (20160224C) Compiled by S.H. C221000100043 ENDBIB 41 0 C221000100044 COMMON 1 3 C221000100045 EN-APRX C221000100046 MEV/A C221000100047 80.0 C221000100048 ENDCOMMON 3 0 C221000100049 ENDSUBENT 48 0 C221000199999 SUBENT C2210002 20160224 C157C221000200001 BIB 2 2 C221000200002 REACTION (5-B-11(50-SN-108,X)50-SN-107,,SIG) C221000200003 STATUS (TABLE) Data taken from tab. 1 of the reference C221000200004 ENDBIB 2 0 C221000200005 NOCOMMON 0 0 C221000200006 DATA 1 1 C221000200007 DATA-MAX C221000200008 MB C221000200009 112. C221000200010 ENDDATA 3 0 C221000200011 ENDSUBENT 10 0 C221000299999 SUBENT C2210003 20160224 C157C221000300001 BIB 3 4 C221000300002 REACTION (5-B-11(50-SN-108,X)50-SN-107,PAR,SIG) C221000300003 ERR-ANALYS (DATA-ERR) Uncertainty includes both statistical and C221000300004 systematic sources C221000300005 STATUS (TABLE) Data taken from tab. 1 of the reference C221000300006 ENDBIB 4 0 C221000300007 NOCOMMON 0 0 C221000300008 DATA 4 3 C221000300009 E-LVL DATA DATA-ERR DATA-MAX C221000300010 KEV MB MB MB C221000300011 0. 52. C221000300012 151. 11. 2. C221000300013 1220. 49. 7. C221000300014 ENDDATA 5 0 C221000300015 ENDSUBENT 14 0 C221000399999 ENDENTRY 3 0 C221099999999