ENTRY C2410 20191103 C188C241000000001 SUBENT C2410001 20191103 C188C241000100001 BIB 11 51 C241000100002 TITLE Inverse-kinematics proton scattering from 42,44S, 41, C241000100003 43P, and the collapse of the N = 28 major shell closureC241000100004 AUTHOR (L.A.Riley,D.Bazin,J.Belarge,P.C.Bender,B.A.Brown, C241000100005 P.D.Cottle,B.Elman,A.Gade,S.D.Gregory,E.B.Haldeman, C241000100006 K.W.Kemper,B.R.Klybor,M.A.Liggett,S.Lipschutz, C241000100007 B.Longfellow,E.Lunderberg,T.Mijatovic,J.Pereira, C241000100008 L.M.Skiles,R.Titus,A.Volya,D.Weisshaar,J.C.Zamora, C241000100009 R.G.T.Zegers) C241000100010 INSTITUTE (1USAURS,1USAMSU,1USAFSU) C241000100011 REFERENCE (J,PR/C,100,044312,2019) C241000100012 FACILITY (CYCTM,1USAMSU) Experiment was performed at the C241000100013 Coupled-Cyclotron Facility of the National C241000100014 Superconducting Cyclotron Laboratory at Michigan C241000100015 State University C241000100016 SAMPLE Liquid hydrogen target located at the target position C241000100017 of the S800. The liquid hydrogen was contained by a C241000100018 cylindrical aluminum target cell, with a 125 mu-m C241000100019 Kapton entrance and exit windows. The nominal target C241000100020 thickness was 30 mm. The temperature and the pressure C241000100021 of the target cell were 17.0 K and 880 Torr. C241000100022 Variations of target thickness caused by pressure C241000100023 difference across Kapton entrance and exit windows C241000100024 were taken into account. Areal density of the target C241000100025 was (240+-2) mg/cm2. C241000100026 DETECTOR (IOCH) Outgoing beam particles were identified by C241000100027 energy loss in the S800 ionization chamber and time C241000100028 of flight. C241000100029 (HPGE) The gamma rays emitted by the reaction products C241000100030 were detected by eight modules of the GRETINA C241000100031 gamma-ray tracking array, centered on the target. C241000100032 Eight modules housing four 36-fold segmented C241000100033 high-purity germanium crystals were installed on one C241000100034 of the GRETINA mounting hemispheres to accommodate C241000100035 the target. Two modules were centered at 58deg, four C241000100036 at 90deg, and two at 122deg with respect to the beam C241000100037 axis. C241000100038 METHOD (TOF) Particles in the secondary beam as well as C241000100039 reaction products were identified using time of flight.C241000100040 INC-SOURCE (KINDT) The secondary beams 42,44S and 41,43P were C241000100041 produced by fragmentation of a 140 MeV/nucleon 48Ca C241000100042 primary beam in a 1222 mg/cm2 9Be production target C241000100043 and separated by the A1900 fragment separator. Two C241000100044 magnet settings of the A1900 were used with momentum C241000100045 acceptance of 2%. Aluminium wedge was used to C241000100046 separate secondary beams by Z. The secondary beams C241000100047 were momentum analysed by S800 spectrograph. C241000100048 Particles were identified by time of flight using C241000100049 scintillation detectors in A1900 focal plane and C241000100050 object and focal plane of S800 spectrograph. C241000100051 ERR-ANALYS (DATA-ERR) Origin of uncertainties not described C241000100052 HISTORY (20191103C) Compiled by S.H. C241000100053 ENDBIB 51 0 C241000100054 NOCOMMON 0 0 C241000100055 ENDSUBENT 54 0 C241000199999 SUBENT C2410002 20191103 C188C241000200001 BIB 2 3 C241000200002 REACTION ((1-H-1(16-S-42,INL)1-H-1,PAR,SIG,G)= C241000200003 (16-S-42(P,INL)16-S-42,PAR,SIG,G)) C241000200004 STATUS (TABLE) Data taken from tab.2 of the reference C241000200005 ENDBIB 3 0 C241000200006 COMMON 1 3 C241000200007 EN C241000200008 MEV/A C241000200009 62.5 C241000200010 ENDCOMMON 3 0 C241000200011 DATA 5 3 C241000200012 E E-ERR DATA DATA-ERR LVL-INI C241000200013 KEV KEV MB MB KEV C241000200014 903. 2. 23. 6. 902. C241000200015 1820. 30. 2.4 1.2 2722. C241000200016 2990. 30. 6.2 1.5 3002. C241000200017 ENDDATA 5 0 C241000200018 ENDSUBENT 17 0 C241000299999 SUBENT C2410003 20191103 C188C241000300001 BIB 2 3 C241000300002 REACTION ((1-H-1(16-S-44,INL)1-H-1,PAR,SIG,G)= C241000300003 (16-S-44(P,INL)16-S-44,PAR,SIG,G)) C241000300004 STATUS (TABLE) Data taken from tab.2 of the reference C241000300005 ENDBIB 3 0 C241000300006 COMMON 1 3 C241000300007 EN C241000300008 MEV/A C241000300009 70.2 C241000300010 ENDCOMMON 3 0 C241000300011 DATA 5 5 C241000300012 E E-ERR DATA DATA-ERR LVL-INI C241000300013 KEV KEV MB MB KEV C241000300014 954. 4. 4.5 0.8 2283. C241000300015 1150. 11. 2.7 0.8 2479. C241000300016 1329. 15. 3. 1329. C241000300017 1899. 6. 3.7 0.7 3264. C241000300018 2698. 13. 2.1 0.5 4027. C241000300019 ENDDATA 7 0 C241000300020 ENDSUBENT 19 0 C241000399999 SUBENT C2410004 20191103 C188C241000400001 BIB 2 3 C241000400002 REACTION ((1-H-1(15-P-41,INL)1-H-1,PAR,SIG,G)= C241000400003 (15-P-41(P,INL)15-P-41,PAR,SIG,G)) C241000400004 STATUS (TABLE) Data taken from tab.2 of the reference C241000400005 ENDBIB 3 0 C241000400006 COMMON 1 3 C241000400007 EN C241000400008 MEV/A C241000400009 57.7 C241000400010 ENDCOMMON 3 0 C241000400011 DATA 5 4 C241000400012 E E-ERR DATA DATA-ERR LVL-INI C241000400013 KEV KEV MB MB KEV C241000400014 173. 1. 6. 2. 173. C241000400015 733. 6. 1.1 0.3 2324. C241000400016 972. 3. 13.5 0.6 1150. C241000400017 1415. 4. 4.6 0.4 1589. C241000400018 ENDDATA 6 0 C241000400019 ENDSUBENT 18 0 C241000499999 SUBENT C2410005 20191103 C188C241000500001 BIB 2 3 C241000500002 REACTION ((1-H-1(15-P-43,INL)1-H-1,PAR,SIG,G)= C241000500003 (15-P-43(P,INL)15-P-43,PAR,SIG,G)) C241000500004 STATUS (TABLE) Data taken from tab.2 of the reference C241000500005 ENDBIB 3 0 C241000500006 COMMON 1 3 C241000500007 EN C241000500008 MEV/A C241000500009 64.7 C241000500010 ENDCOMMON 3 0 C241000500011 DATA 5 4 C241000500012 E E-ERR DATA DATA-ERR LVL-INI C241000500013 KEV KEV MB MB KEV C241000500014 188. 1. 4. 2. 188. C241000500015 827. 4. 6.2 1.2 1015. C241000500016 846. 11. 4.9 1.4 845. C241000500017 916. 5. 3.5 0.8 1104. C241000500018 ENDDATA 6 0 C241000500019 ENDSUBENT 18 0 C241000599999 ENDENTRY 5 0 C241099999999