ENTRY C2699 20211209 C211C269900000001 SUBENT C2699001 20211209 C211C269900100001 BIB 10 43 C269900100002 TITLE Spectroscopy of the T=2mirror nuclei 48Fe/48Ti using C269900100003 mirrored knockout reactions C269900100004 AUTHOR (R.Yajzey,M.A.Bentley,E.C.Simpson,T.Haylett, C269900100005 S.Uthayakumaar,D.Bazin,J.Belarge,P.C.Bender, C269900100006 P.J.Davies,B.Elman,A.Gade,H.Iwasaki,D.Kahl, C269900100007 N.Kobayashi,S.M.Lenzi,B.Longfellow,S.J.Lonsdale, C269900100008 E.Lunderberg,L.Morris,D.R.Napoli,X.Pereira-Lopez, C269900100009 F.Recchia,J.A.Tostevin,R.Wadsworth,D.Weisshaar) C269900100010 INSTITUTE (2UK YRK,3AULCBR,1USAMSU,2UK EDG,2ITYPAD,2UK SUR, C269900100011 3RUMBUC) C269900100012 (3SARSAR) Jazan University, Jazan C269900100013 REFERENCE (J,PL/B,823,136757,2021) C269900100014 FACILITY (CYCLO,1USAMSU) experiment was performed at the C269900100015 National Superconducting Cyclotron Laboratory C269900100016 at Michigan State University. C269900100017 SAMPLE 9Be reaction target with thickness of 188 mg/cm2 C269900100018 INC-SOURCE The 58Ni primary beam was accelerated through C269900100019 the K500/K1200 cyclotrons to an energy 160MeV/A C269900100020 and fragmented on a 802 mg/cm2 9Be production target. C269900100021 Fragments were separated by the A1900 separator C269900100022 into a cocktail beam that contained 49Fe in one C269900100023 setting of the A1900 and 49V in another. The fragment C269900100024 beam rates for 49Fe was 300 pps and for 49V beam rate C269900100025 was 2E+5 particles per second. The secondary beams C269900100026 were identified by measuring their time of flight C269900100027 between two plastic scintillator detectors, one C269900100028 located after the A1900 fragment separator and the C269900100029 other in the S800 analysis beam line. C269900100030 METHOD (TOFDE) Identification of reaction products C269900100031 DETECTOR (MAGSP,IOCH,SCIN) Reaction products were identified C269900100032 in the S800 by measuring the energy loss in an C269900100033 ionization chamber in conjunction with ToF measured C269900100034 between scintillators in the beam line C269900100035 (HPGE) The gamma rays were measured using the C269900100036 gamma-ray array GRETINA, consisting of nine detector C269900100037 modules, each comprising four high-purity germanium C269900100038 crystals. Four of these modules were centred at 58 deg C269900100039 and five centred at 90 deg in relation to the beam C269900100040 direction. To maximise photopeak efficiency and C269900100041 optimise the coincidence analysis, an add-back C269900100042 procedure was applied in which energies deposited C269900100043 in neighbouring GRETINA crystals were summed C269900100044 HISTORY (20211128C) Compiled by S.H. C269900100045 ENDBIB 43 0 C269900100046 NOCOMMON 0 0 C269900100047 ENDSUBENT 46 0 C269900199999 SUBENT C2699002 20211209 C211C269900200001 BIB 5 14 C269900200002 REACTION ((4-BE-9(26-FE-49,X)26-FE-48,PAR,SIG)= C269900200003 (26-FE-49(4-BE-9,X)26-FE-48,PAR,SIG)) C269900200004 PART-DET (G,26-FE-48) C269900200005 LEVEL-PROP (26-FE-48,E-LVL=0.971,SPIN=2.,PARITY=+1.) C269900200006 (26-FE-48,E-LVL=2.255,SPIN=4.,PARITY=+1.) C269900200007 (26-FE-48,E-LVL=2.378,SPIN=2.,PARITY=+1.) C269900200008 (26-FE-48,E-LVL=3.200,SPIN=4.,PARITY=+1.) C269900200009 (26-FE-48,E-LVL=3.244,SPIN=6.,PARITY=+1.) C269900200010 (26-FE-48,E-LVL=3.476,SPIN=3.,PARITY=-1.) C269900200011 (26-FE-48,E-LVL=3.500,SPIN=6.,PARITY=+1.) C269900200012 (26-FE-48,E-LVL=4.206,SPIN=5.,PARITY=-1.) C269900200013 ERR-ANALYS (DATA-ERR) Total uncertainty including statistical C269900200014 and systematic uncertainty C269900200015 STATUS (TABLE) Data taken from the tab.1 of the reference. C269900200016 ENDBIB 14 0 C269900200017 COMMON 1 3 C269900200018 EN C269900200019 MEV/A C269900200020 80. C269900200021 ENDCOMMON 3 0 C269900200022 DATA 3 9 C269900200023 E-LVL DATA DATA-ERR C269900200024 KEV MB MB C269900200025 0. 3. 2. C269900200026 971. 0.9 0.9 C269900200027 2255. 1.1 0.8 C269900200028 2378. 0.4 0.2 C269900200029 3200. 0.5 0.4 C269900200030 3244. 0.1 0.6 C269900200031 3476. 0.4 0.2 C269900200032 3500. 1.9 0.4 C269900200033 4206. 0.3 0.2 C269900200034 ENDDATA 11 0 C269900200035 ENDSUBENT 34 0 C269900299999 SUBENT C2699003 20211209 C211C269900300001 BIB 5 17 C269900300002 REACTION ((4-BE-9(22-TI-49,X)22-TI-48,PAR,SIG)= C269900300003 (22-TI-49(4-BE-9,X)22-TI-48,PAR,SIG)) C269900300004 PART-DET (G,22-TI-48) C269900300005 LEVEL-PROP (22-TI-48,E-LVL=0.983,SPIN=2.,PARITY=+1.) C269900300006 (22-TI-48,E-LVL=2.295,SPIN=4.,PARITY=+1.) C269900300007 (22-TI-48,E-LVL=2.420,SPIN=2.,PARITY=+1.) C269900300008 (22-TI-48,E-LVL=3.223,SPIN=3.,PARITY=+1.) C269900300009 (22-TI-48,E-LVL=3.239,SPIN=4.,PARITY=+1.) C269900300010 (22-TI-48,E-LVL=3.332,SPIN=6.,PARITY=+1.) C269900300011 (22-TI-48,E-LVL=3.358,SPIN=3.,PARITY=-1.) C269900300012 (22-TI-48,E-LVL=3.507,SPIN=6.,PARITY=+1.) C269900300013 (22-TI-48,E-LVL=3.781,SPIN=3./4.,PARITY=-1.) C269900300014 (22-TI-48,E-LVL=3.851,SPIN=3.,PARITY=+1.) C269900300015 (22-TI-48,E-LVL=4.045,SPIN=5.,PARITY=-1.) C269900300016 ERR-ANALYS (DATA-ERR) Total uncertainty including statistical C269900300017 and systematic uncertainty C269900300018 STATUS (TABLE) Data taken from the tab.1 of the reference. C269900300019 ENDBIB 17 0 C269900300020 COMMON 1 3 C269900300021 EN C269900300022 MEV/A C269900300023 84. C269900300024 ENDCOMMON 3 0 C269900300025 DATA 3 12 C269900300026 E-LVL DATA DATA-ERR C269900300027 KEV MB MB C269900300028 0. 18. 3. C269900300029 983. 4. 2. C269900300030 2295. 13. 2. C269900300031 2420. 3.2 0.4 C269900300032 3223. 1.2 0.3 C269900300033 3239. 2.8 0.4 C269900300034 3332. 8.3 0.9 C269900300035 3358. 4.6 0.6 C269900300036 3507. 7.2 0.7 C269900300037 3781. 2.5 0.3 C269900300038 3851. 4.2 0.6 C269900300039 4045. 0.3 0.2 C269900300040 ENDDATA 14 0 C269900300041 ENDSUBENT 40 0 C269900399999 SUBENT C2699004 20211209 C211C269900400001 BIB 3 4 C269900400002 REACTION ((4-BE-9(26-FE-49,X)26-FE-48,,SIG)= C269900400003 (26-FE-49(4-BE-9,X)26-FE-48,,SIG)) C269900400004 ERR-ANALYS (DATA-ERR) Origin of uncertainties not described C269900400005 STATUS (TABLE) Data taken from the tab.1 of the reference. C269900400006 ENDBIB 4 0 C269900400007 NOCOMMON 0 0 C269900400008 DATA 3 1 C269900400009 EN DATA DATA-ERR C269900400010 MEV/A MB MB C269900400011 80. 8. 2. C269900400012 ENDDATA 3 0 C269900400013 ENDSUBENT 12 0 C269900499999 SUBENT C2699005 20211209 C211C269900500001 BIB 3 4 C269900500002 REACTION ((4-BE-9(22-TI-49,X)22-TI-48,,SIG)= C269900500003 (22-TI-49(4-BE-9,X)22-TI-48,,SIG)) C269900500004 ERR-ANALYS (DATA-ERR) Origin of uncertainties not described C269900500005 STATUS (TABLE) Data taken from the tab.1 of the reference. C269900500006 ENDBIB 4 0 C269900500007 NOCOMMON 0 0 C269900500008 DATA 3 1 C269900500009 EN DATA DATA-ERR C269900500010 MEV/A MB MB C269900500011 84. 74. 6. C269900500012 ENDDATA 3 0 C269900500013 ENDSUBENT 12 0 C269900599999 ENDENTRY 5 0 C269999999999