ENTRY C2382 20190606 C186C238200000001 SUBENT C2382001 20190606 C186C238200100001 BIB 10 40 C238200100002 TITLE Shape coexistence and mixing of low-lying 0+ states C238200100003 in 96Sr C238200100004 AUTHOR (S.Cruz,P.C.Bender,R.Krucken,K.Wimmer,F.Ames, C238200100005 C.Andreoiu,R.A.E.Austin,C.S.Bancroft,R.Braid,T.Bruhn, C238200100006 W.N.Catford,A.Cheeseman,A.Chester,D.S.Cross,C.Aa.Diget,C238200100007 T.Drake,A.B.Garnsworthy,G.Hackman,R.Kanungo,A.Knapton, C238200100008 W.Korten,K.Kuhn,J.Lassen,R.Laxdal,M.Marchetto,A.Matta, C238200100009 D.Miller,M.Moukaddam,N.A.Orr,N.Sachmpazidi, C238200100010 A.Sanetullaev,C.E.Svensson,N.Terpstra,C.Unsworth, C238200100011 P.J.Voss) C238200100012 INSTITUTE (1CANUBC,1CANTMF,2JPNTOK,1CANSFU,1CANSMR,2UK SUR, C238200100013 2UK YRK,1CANTOR,2FR SAC,1CANGUE) C238200100014 (1USAUSA)Central Michigan University, Mt Pleasant C238200100015 (2FR FR) Normandie Universite, Caen C238200100016 REFERENCE (J,PL/B,786,94,2018) C238200100017 FACILITY (LINAC,1CANTMF) Experiment was performed at the C238200100018 TRIUMF-ISAC2 facility C238200100019 SAMPLE (1-H-2,ENR=0.92) The beam impinged upon a 0.44+-0.04 C238200100020 mg/cm2, deuterated polyethylene (CD2) target C238200100021 DETECTOR (SISD) Deuterated target was mounted in the center of C238200100022 the SHARC silicon detector array. SHARC (Silicon C238200100023 Highly-segmented Array for Reactions and Coulex) is a C238200100024 compact arrangement of double-sided silicon strip C238200100025 detectors which is optimized for high geometrical C238200100026 efficiency and excellent spatial resolution. C238200100027 (HPGE) The SHARC array was surrounded by the TIGRESS C238200100028 gamma-ray detector array, with 12 HPGe C238200100029 Compton-suppressed clover detectors arranged in a C238200100030 com- pact hemispherical arrangement with C238200100031 approximately 50% of 4PI geometrical coverage C238200100032 INC-SOURCE 95Sr beam was produced by impinging a 480 MeV proton C238200100033 beam with an intensity of 10 mu-Aon a UCx target. The C238200100034 neutron-rich Sr isotopes were produced through C238200100035 uranium fission, were laser ionized, mass separated C238200100036 and transported to a charge state booster. The beam C238200100037 (Q=16+) was transported to the ISAC2 facility where C238200100038 its kinetic energy was increased to 5.5AMeV using the C238200100039 superconducting linear accelerator C238200100040 ERR-ANALYS (DATA-ERR) Sources of uncertainties not described. C238200100041 HISTORY (20181216C) Compiled by S.H. C238200100042 ENDBIB 40 0 C238200100043 COMMON 1 3 C238200100044 EN C238200100045 MEV/A C238200100046 5.5 C238200100047 ENDCOMMON 3 0 C238200100048 ENDSUBENT 47 0 C238200199999 SUBENT C2382002 20190606 C186C238200200001 BIB 2 4 C238200200002 REACTION ((1-H-2(38-SR-95,P)38-SR-96,PAR,DA,RSD)= C238200200003 (38-SR-95(D,P)38-SR-96,PAR,DA)) C238200200004 STATUS (TABLE) Data presented in fig.3a of the reference C238200200005 sent by author (K.W.) C238200200006 ENDBIB 4 0 C238200200007 COMMON 1 3 C238200200008 E-LVL C238200200009 KEV C238200200010 0. C238200200011 ENDCOMMON 3 0 C238200200012 DATA 3 32 C238200200013 ANG-CM DATA-CM DATA-ERR C238200200014 ADEG MB/SR MB/SR C238200200015 3. 1.24189 0.168169 C238200200016 5. 1.65549 0.167942 C238200200017 7. 1.42136 0.166185 C238200200018 9. 1.34221 0.162677 C238200200019 11. 0.69519 0.112475 C238200200020 13. 0.361006 0.0494068 C238200200021 17. 0.195647 0.0948989 C238200200022 19. 0.172909 0.0681887 C238200200023 21. 0.252832 0.0599348 C238200200024 23. 0.408053 0.0539276 C238200200025 25. 0.394719 0.0637026 C238200200026 27. 0.532291 0.058271 C238200200027 29. 0.442421 0.054781 C238200200028 31. 0.557532 0.0504281 C238200200029 33. 0.487649 0.0465608 C238200200030 35. 0.445011 0.0426602 C238200200031 37. 0.353654 0.0400137 C238200200032 39. 0.276725 0.0341969 C238200200033 41. 0.252722 0.0499266 C238200200034 43. 0.150453 0.0302594 C238200200035 45. 0.137603 0.0168453 C238200200036 65. 0.0856606 0.0424439 C238200200037 67. 0.154615 0.0318008 C238200200038 69. 0.170283 0.028947 C238200200039 71. 0.114876 0.0285427 C238200200040 73. 0.115583 0.0207952 C238200200041 75. 0.135633 0.0242438 C238200200042 77. 0.117795 0.0206228 C238200200043 79. 0.0801373 0.0220164 C238200200044 81. 0.0874179 0.0210581 C238200200045 83. 0.0608104 0.0157919 C238200200046 85. 0.0496815 0.0147662 C238200200047 ENDDATA 34 0 C238200200048 ENDSUBENT 47 0 C238200299999 SUBENT C2382003 20190606 C186C238200300001 BIB 2 4 C238200300002 REACTION ((1-H-2(38-SR-95,P)38-SR-96,PAR,DA,RSD)= C238200300003 (38-SR-95(D,P)38-SR-96,PAR,DA)) C238200300004 STATUS (TABLE) Data presented in fig.3b of the reference C238200300005 sent by author (K.W.) C238200300006 ENDBIB 4 0 C238200300007 COMMON 1 3 C238200300008 E-LVL C238200300009 KEV C238200300010 1229. C238200300011 ENDCOMMON 3 0 C238200300012 DATA 3 22 C238200300013 ANG-CM DATA-CM DATA-ERR C238200300014 ADEG MB/SR MB/SR C238200300015 4.5 2.4326 0.263627 C238200300016 7.5 1.45115 0.186712 C238200300017 10.5 1.39466 0.140878 C238200300018 16.5 0.298406 0.0579969 C238200300019 19.5 0.218053 0.0363742 C238200300020 22.5 0.393438 0.0475647 C238200300021 25.5 0.584621 0.0544332 C238200300022 28.5 0.703303 0.0620912 C238200300023 31.5 0.775662 0.0592826 C238200300024 34.5 0.751368 0.0617235 C238200300025 37.5 0.644522 0.0586222 C238200300026 40.5 0.451211 0.0441833 C238200300027 43.5 0.27038 0.0560521 C238200300028 64.5 0.13864 0.0373556 C238200300029 67.5 0.217911 0.0348529 C238200300030 70.5 0.203779 0.031877 C238200300031 73.5 0.203952 0.0324702 C238200300032 76.5 0.18782 0.0260357 C238200300033 79.5 0.170009 0.0243611 C238200300034 82.5 0.145353 0.0214977 C238200300035 85.5 0.132157 0.0202189 C238200300036 88.5 0.0893597 0.0159063 C238200300037 ENDDATA 24 0 C238200300038 ENDSUBENT 37 0 C238200399999 ENDENTRY 3 0 C238299999999