ENTRY C2401 20190821 C188C240100000001 SUBENT C2401001 20190821 C188C240100100001 BIB 12 35 C240100100002 TITLE One-proton and one-neutron knockout reactions from C240100100003 N=Z=28 56Ni to the A = 55 mirror pair 55Co and 55Ni C240100100004 AUTHOR (M.Spieker,A.Gade,D.Weisshaar,B.A.Brown,J.A.Tostevin, C240100100005 B.Longfellow,P.Adrich,D.Bazin,M.A.Bentley,J.R.Brown, C240100100006 C.M.Campbell,C.Aa.Diget,B.Elman,T.Glasmacher,M.Hill, C240100100007 B.Pritychenko,A.Ratkiewicz,D.Rhodes) C240100100008 INSTITUTE (1USAMSU,2UK SUR,2UK YRK,1USABNL) C240100100009 REFERENCE (J,PR/C,99,051304,2019) C240100100010 FACILITY (CYCTM,1USAMSU) The experiment was performed at the C240100100011 Coupled Cyclotron Facility of the National C240100100012 Superconducting Cyclotron Laboratory at Michigan C240100100013 State University C240100100014 SAMPLE 9Be reaction target with thickness of 188 mg/cm2 C240100100015 DETECTOR (HPGE) Gamma rays were detected by SEGA array C240100100016 consisting of 16 32-fold segmented HPGe detectors. C240100100017 The detectors were arranged in two rings with central C240100100018 angles of 37deg and 90 deg. C240100100019 (MAGSP) Projectile-like reaction residues were C240100100020 momentum-analysed in S800 spectrometer and identified C240100100021 event-by-event in focal plane detector. C240100100022 CORRECTION All gamma ray energies were Doppler corrected using C240100100023 information from HPGe detector segment and momentum of C240100100024 reaction residues. C240100100025 METHOD (TOF,EDE) C240100100026 INC-SOURCE (KINDT) The secondary 56Ni beam was produced by C240100100027 projectile fragmentation of 160 MeV/A 58Ni primary C240100100028 beam on a thick 610 mg/cm2 9Be target. The 56Ni C240100100029 secondary beam was analysed using A1900 fragment C240100100030 separator and was unambiguously distinguished from C240100100031 all contaminants via the time-of-flight difference C240100100032 measured between two plastic scintillators located at C240100100033 the exit of the A1900 and the object position of the C240100100034 S800 analysis beam line. C240100100035 ERR-ANALYS (ERR-S) Statistical uncertainty C240100100036 HISTORY (20190821C) Compiled by S.H. C240100100037 ENDBIB 35 0 C240100100038 COMMON 1 3 C240100100039 EN C240100100040 MEV/A C240100100041 160. C240100100042 ENDCOMMON 3 0 C240100100043 ENDSUBENT 42 0 C240100199999 SUBENT C2401002 20190821 C188C240100200001 BIB 2 3 C240100200002 REACTION (4-BE-9(28-NI-56,X)28-NI-55,PAR,SIG) C240100200003 STATUS (TABLE) Data presented in fig 3a of the reference C240100200004 sent by author (M.-Ch.S.) C240100200005 ENDBIB 3 0 C240100200006 NOCOMMON 0 0 C240100200007 DATA 3 8 C240100200008 E-LVL DATA ERR-S C240100200009 KEV MB MB C240100200010 2086. 1.84 0.1 C240100200011 2466. 0.11 0.09 C240100200012 2587. 0.71 0.08 C240100200013 2842. 0.62 0.1 C240100200014 2882. 1.42 0.1 C240100200015 3186. 2.32 0.1 C240100200016 3218. 0.38 0.09 C240100200017 3759. 1.49 0.06 C240100200018 ENDDATA 10 0 C240100200019 ENDSUBENT 18 0 C240100299999 SUBENT C2401003 20190821 C188C240100300001 BIB 2 3 C240100300002 REACTION (4-BE-9(28-NI-56,X)27-CO-55,PAR,SIG) C240100300003 STATUS (TABLE) Data presented in fig 3b of the reference C240100300004 sent by author (M.-Ch.S.) C240100300005 ENDBIB 3 0 C240100300006 NOCOMMON 0 0 C240100300007 DATA 3 11 C240100300008 E-LVL DATA ERR-S C240100300009 KEV MB MB C240100300010 2166. 2.9 0.3 C240100300011 2566. 2.8 0.4 C240100300012 2660. 4. 0.2 C240100300013 2919. 3.8 0.2 C240100300014 2923. 8.3 0.4 C240100300015 2939. 2.5 0.2 C240100300016 2960. 2.4 0.2 C240100300017 2976. 8.2 0.3 C240100300018 3303. 1.8 0.4 C240100300019 3323. 2.4 0.6 C240100300020 3565. 6.1 0.4 C240100300021 ENDDATA 13 0 C240100300022 ENDSUBENT 21 0 C240100399999 ENDENTRY 3 0 C240199999999