ENTRY C2383 20190606 C186C238300000001 SUBENT C2383001 20190606 C186C238300100001 BIB 12 50 C238300100002 TITLE Neutron-hole states in 131Sn and spin-orbit splitting C238300100003 in neutron-rich nuclei C238300100004 AUTHOR (R.Orlandi,S.D.Pain,S.Ahn,A.Jungclaus,K.T.Schmitt, C238300100005 D.W.Bardayan,W.N.Catford,R.Chapman,K.A.Chipps, C238300100006 J.A.Cizewski,C.G.Gross,M.E.Howard,K.L.Jones,R.L.Kozub, C238300100007 B.Manning,M.Matos,K.Nishio,P.D.O'Malley,W.A.Peters, C238300100008 S.T.Pittman,A.Ratkiewicz,C.Shand,J.F.Smith,M.S.Smith, C238300100009 T.Fukui,J.A.Tostevin,Y.Utsuno) C238300100010 INSTITUTE (2JPNJAE,2SPNIEM,1USAORL,1USATEN,2UK SUR,1USACSM, C238300100011 1USARUT,1USATTU,1USALSU,1USAOAU,2ITYNAP,2JPNTIT) C238300100012 (2UK UK) University of the West of Scotland, Paisley C238300100013 (2UK UK) The Scottish Universities Physics Alliance C238300100014 REFERENCE (J,PL/B,785,615,2018) C238300100015 FACILITY (VDGT,1USAORL) Present experiment was performed at C238300100016 the Holifield Radioactive Ion Beam Facility (HRIBF) C238300100017 at Oak Ridge National Laboratory. C238300100018 SAMPLE Deuterated polyethylene (C2D4) sample was used. Two C238300100019 targets were used: the initial 214 mu-g/cm2-thick C238300100020 film was replaced after 40 hours of beamtime with a C238300100021 thicker 350 mu-g/cm2 target. C238300100022 DETECTOR (TELES,SISD,SISD) The SuperORRUBA array of segmented C238300100023 Si telescopes was used to detect tritons from the C238300100024 (d,t) reaction. The array comprised of seven E-dE C238300100025 telescopes from the ORRUBA array to identify the C238300100026 light ejectiles and four additional E detectors to C238300100027 monitor elastically-scattered deuterons for beam C238300100028 normalization. The respective thickness was 65 mu-m C238300100029 for dE and 1000 mu-m for E detectors. The telescopes C238300100030 were placed at a radial distance of 123 mm from the C238300100031 target. The large segmentation of the E detectors (64 C238300100032 strips perpendicular to the beam direction) combined C238300100033 with the 8-fold segmentation (parallel to the beam C238300100034 direction) of the E detectors, resulted in an average C238300100035 resolution of 0.28 degrees in polar angle. The C238300100036 angular range covered by the telescopes and two of C238300100037 the E detectors was 35 - 50 degrees in the laboratory C238300100038 frame, while the two remaining E detectors were C238300100039 placed close to 90 degrees. C238300100040 METHOD (EDE) C238300100041 INC-SOURCE The radioactive 132Sn beam was produced via the C238300100042 proton-induced fission of 238U in a UCx target, C238300100043 extracted using the isotope separation online (ISOL) C238300100044 technique, and accelerated by the 25-MV ORNL Tandem C238300100045 electrostatic accelerator to 580 MeV. C238300100046 ANALYSIS The triton angular distributions were converted to C238300100047 absolute cross sections using the normalization C238300100048 determined from the elastic scattering of deuterons C238300100049 from the same target C238300100050 ERR-ANALYS (DATA-ERR) Source of uncertainties not described C238300100051 HISTORY (20181217C) Compiled by S.H. C238300100052 ENDBIB 50 0 C238300100053 COMMON 1 3 C238300100054 EN C238300100055 MEV/A C238300100056 4.4 C238300100057 ENDCOMMON 3 0 C238300100058 ENDSUBENT 57 0 C238300199999 SUBENT C2383002 20190612 C186C238300200001 BIB 2 4 C238300200002 REACTION ((1-H-2(50-SN-132,T)50-SN-131,PAR,DA,RSD)= C238300200003 (50-SN-132(D,T)50-SN-131,PAR,DA)) C238300200004 STATUS (TABLE) Data presented in fig. 3 of the reference C238300200005 sent by R.O. C238300200006 ENDBIB 4 0 C238300200007 COMMON 2 3 C238300200008 E-LVL E-LVL C238300200009 KEV KEV C238300200010 0. 65. C238300200011 ENDCOMMON 3 0 C238300200012 DATA 4 4 C238300200013 ANG-CM ANG-ERR DATA-CM DATA-ERR C238300200014 ADEG ADEG MB/SR MB/SR C238300200015 54.43 8.06 1.21 0.16 C238300200016 67.79 5.38 1.20 0.23 C238300200017 77.29 4.22 1.72 0.28 C238300200018 85.03 3.53 1.72 0.33 C238300200019 ENDDATA 6 0 C238300200020 ENDSUBENT 19 0 C238300299999 SUBENT C2383003 20190606 C186C238300300001 BIB 2 4 C238300300002 REACTION ((1-H-2(50-SN-132,T)50-SN-131,PAR,DA,RSD)= C238300300003 (50-SN-132(D,T)50-SN-131,PAR,DA)) C238300300004 STATUS (TABLE) Data presented in fig. 3 of the reference C238300300005 sent by R.O. C238300300006 ENDBIB 4 0 C238300300007 COMMON 1 3 C238300300008 E-LVL C238300300009 KEV C238300300010 332. C238300300011 ENDCOMMON 3 0 C238300300012 DATA 4 4 C238300300013 ANG-CM ANG-ERR DATA-CM DATA-ERR C238300300014 ADEG ADEG MB/SR MB/SR C238300300015 51.04 9.70 1.08 0.16 C238300300016 66.49 5.75 1.31 0.23 C238300300017 76.43 4.35 1.70 0.27 C238300300018 84.35 3.59 1.52 0.30 C238300300019 ENDDATA 6 0 C238300300020 ENDSUBENT 19 0 C238300399999 SUBENT C2383004 20190606 C186C238300400001 BIB 2 4 C238300400002 REACTION ((1-H-2(50-SN-132,T)50-SN-131,PAR,DA,RSD)= C238300400003 (50-SN-132(D,T)50-SN-131,PAR,DA)) C238300400004 STATUS (TABLE) Data presented in fig. 3 of the reference C238300400005 sent by R.O. C238300400006 ENDBIB 4 0 C238300400007 COMMON 1 3 C238300400008 E-LVL C238300400009 KEV C238300400010 1654. C238300400011 ENDCOMMON 3 0 C238300400012 DATA 4 3 C238300400013 ANG-CM ANG-ERR DATA-CM DATA-ERR C238300400014 ADEG ADEG MB/SR MB/SR C238300400015 46.00 8.00 0.16 0.081 C238300400016 62.74 8.80 0.13 0.050 C238300400017 74.73 4.84 0.16 0.082 C238300400018 ENDDATA 5 0 C238300400019 ENDSUBENT 18 0 C238300499999 ENDENTRY 4 0 C238399999999