ENTRY C2291 20180131 C175C229100000001 SUBENT C2291001 20180131 C175C229100100001 BIB 10 45 C229100100002 TITLE Spectroscopy of 54Ti and the systematic behavior of C229100100003 low-energy octupole states in Ca and Ti isotopes C229100100004 AUTHOR (L.A.Riley,M.L.Agiorgousis,T.R.Baugher,D.Bazin, C229100100005 R.L.Blanchard,M.Bowry,P.D.Cottle,F.G.Devone,A.Gade, C229100100006 M.T.Glowacki,K.W.Kemper,J.S.Kustina,E.Lunderberg, C229100100007 D.M.McPherson,S.Noji,J.Piekarewicz,F.Recchia, C229100100008 B.V.Sadler,M.Scott,D.Weisshaar,R.G.T.Zegers) C229100100009 INSTITUTE (1USAURS,1USAMSU,1USAFSU) C229100100010 REFERENCE (J,PR/C,96,064315,2017) C229100100011 FACILITY (CYCTM,1USAMSU) The experiment was performed at the C229100100012 Coupled-Cyclotron Facility of the National C229100100013 Superconducting Cyclotron Laboratory at Michigan C229100100014 State University C229100100015 SAMPLE Liquid Hydrogen target was used. The liquid hydrogen C229100100016 was contained by a cylindrical aluminum target cell C229100100017 with 125 mu-m Kapton entrance and exit windows mounted C229100100018 on a cryocooler. The nominal target thickness was 30 C229100100019 mm.The effective thickness of the target was C229100100020 determined to be 258 mg/cm2 and mid-target beam C229100100021 energy was 91.5 MeV/nucleon. C229100100022 DETECTOR (SIBAR) Secondary beam particles were identified C229100100023 upstream of the reaction target by energy loss in a C229100100024 silicon surface barrier detector and by time of C229100100025 flight from the A1900 extended focal plane to the C229100100026 S800 object scintillator C229100100027 (MAGSP) Charged reaction products were momentum C229100100028 analysed using magnetic spectrometer S800. C229100100029 (HPGE) The GRETINA gamma-ray tracking array, C229100100030 consisting of 28 36-fold segmented high purity C229100100031 germanium crystals packaged in seven clusters of four C229100100032 crystals each, was installed at the pivot point of C229100100033 the S800 C229100100034 (SCIN) Beamlike reaction products were identified C229100100035 downstream of the target by energy loss in the S800 C229100100036 ion chamber and time of flight from the S800 object C229100100037 scintillator to a scintillator in the focal plane of C229100100038 the S800 C229100100039 METHOD (TOF) Reaction products were identified using time of C229100100040 flight C229100100041 Inverse kinematics was used C229100100042 INC-SOURCE The secondary beam 54Ti was produced by the C229100100043 fragmentation of a 130 MeV/u 76Ge primary beam in a C229100100044 376 mg/cm2 9Be production target and separated by the C229100100045 A1900 fragment separator C229100100046 HISTORY (20180131C) Compiled by S.H. C229100100047 ENDBIB 45 0 C229100100048 NOCOMMON 0 0 C229100100049 ENDSUBENT 48 0 C229100199999 SUBENT C2291002 20180131 C175C229100200001 BIB 4 5 C229100200002 REACTION ((1-H-1(22-TI-54,INL)1-H-1,PAR,SIG,G)= C229100200003 (22-TI-54(P,INL)22-TI-54,PAR,SIG,G)) C229100200004 STATUS (TABLE) Data taken from tab.1 of the reference C229100200005 ERR-ANALYS (DATA-ERR) Origin of uncertainties not described C229100200006 MISC-COL (MISC) Energy of initial level C229100200007 ENDBIB 5 0 C229100200008 COMMON 1 3 C229100200009 EN C229100200010 MEV/A C229100200011 91.5 C229100200012 ENDCOMMON 3 0 C229100200013 DATA 7 4 C229100200014 E E-ERR MISC MISC-ERR DATA DATA-ERR C229100200015 DATA-MAX C229100200016 KEV KEV KEV KEV MB MB C229100200017 MB C229100200018 1000. 3. 2497.4 0.4 3.3 0.4 C229100200019 C229100200020 1022. 3. 2517.1 0.3 C229100200021 0.7 C229100200022 1264. 3. 3780. 3. 4.9 0.4 C229100200023 C229100200024 1495. 2. 1495.0 0.3 8.7 0.8 C229100200025 C229100200026 ENDDATA 12 0 C229100200027 ENDSUBENT 26 0 C229100299999 ENDENTRY 2 0 C229199999999