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