ENTRY 14841 20241015 15171484100000001 SUBENT 14841001 20241015 15171484100100001 BIB 9 35 1484100100002 TITLE Beta-delayed neutron emission of 64Mn, 62Cr, and 65Fe 1484100100003 AUTHOR (W.-J.Ong,H.Schatz,K.Kravvaris,S.Ahn,K.Childers, 1484100100004 B.P.Crider,A.C.Dombos,C.Langer, R.Lewis,S.N.Liddick, 1484100100005 S.Lyons,Z.Meisel,F.Montes,J.Pereira,D.Richman, 1484100100006 K.Schmidt,A.Spyrou) 1484100100007 REFERENCE (J,PR/C,110,024321,2024) 1484100100008 #doi:10.1103/PhysRevC.110.024321 1484100100009 INSTITUTE (1USALRL,1USAMSU,1USATAM,1USAMSS,2GERFRK,1USAOHO, 1484100100010 1USALAS,2GERZFK) 1484100100011 FACILITY (CYCLO,1USAMSU) The National Superconducting 1484100100012 Cyclotron Laboratory (NSCL) at Michigan State 1484100100013 University. 1484100100014 DETECTOR (LONGC,SI,NAICR) The Neutron Emission Ratio Observer 1484100100015 (NERO) neutron long counter system and the Beta 1484100100016 Counting Station (BCS). A stack of two Si PIN 1484100100017 detectors and an Al degrader on a rotating holder, 1484100100018 the Summing NaI detector. 1484100100019 METHOD (TOF) A 35 p nA 82Se beam with an energy of 140 MeV/u 1484100100020 was impinged on a 352 mg/cm2 beryllium target. After 1484100100021 fragmentation, cocktail beam consisted almost 1484100100022 entirely of 61V (24%), 62Cr (19%), 64Mn (51%), and 1484100100023 65Fe (6%). For Beam particles were identified using 1484100100024 the E-TOF (time of flight) method, with the energy loss1484100100025 taken from a 525-microm thick Si PIN detector located 1484100100026 at the beginning of the end station, and the time of 1484100100027 flight calculated from the time difference between an 1484100100028 I2 scintillator at the image position of the A1900 and 1484100100029 the PIN detector. The beam was implanted in a 1484100100030 979-microm thick double-sided silicon strip detector 1484100100031 (DSSD) as part of the BCS. Neutrons detected by NERO 1484100100032 and the beta by BCS in the 200 microsec following a 1484100100033 decay event were considered to be associated with the 1484100100034 beta decay. 1484100100035 CORRECTION Momentum-corrected particle identification. 1484100100036 HISTORY (20241015C) BP 1484100100037 ENDBIB 35 0 1484100100038 NOCOMMON 0 0 1484100100039 ENDSUBENT 38 0 1484100199999 SUBENT 14841002 20241015 15171484100200001 BIB 4 7 1484100200002 REACTION (25-MN-64(0,B-)26-FE-64,,PN) 1484100200003 REL-REF (D,,M.W.Hannawald,T,HANNAWALD,2000) 1484100200004 (A,,D.Pauwels+,J,PR/C,86,064318,2012) 1484100200005 ERR-ANALYS (DATA-ERR) Combination of statistical and large 1484100200006 systematic uncertainties. 1484100200007 STATUS (TABLE,,W.-J.Ong+,J,PR/C,110,024321,2024) 1484100200008 page 024321-3 of J,PR/C,110,024321,2024. 1484100200009 ENDBIB 7 0 1484100200010 NOCOMMON 0 0 1484100200011 DATA 2 1 1484100200012 DATA DATA-ERR 1484100200013 NO-DIM NO-DIM 1484100200014 0.015 0.006 1484100200015 ENDDATA 3 0 1484100200016 ENDSUBENT 15 0 1484100299999 SUBENT 14841003 20241015 15171484100300001 BIB 3 4 1484100300002 REACTION (24-CR-62(0,B-)25-MN-62,,PN) 1484100300003 ERR-ANALYS No information on uncertainties. 1484100300004 STATUS (TABLE,,W.-J.Ong+,J,PR/C,110,024321,2024) 1484100300005 page 024321-3 of J,PR/C,110,024321,2024. 1484100300006 ENDBIB 4 0 1484100300007 NOCOMMON 0 0 1484100300008 DATA 1 1 1484100300009 DATA-MAX 1484100300010 NO-DIM 1484100300011 0.01 1484100300012 ENDDATA 3 0 1484100300013 ENDSUBENT 12 0 1484100399999 SUBENT 14841004 20241015 15171484100400001 BIB 3 4 1484100400002 REACTION (26-FE-65(0,B-)26-FE-65,,PN) 1484100400003 ERR-ANALYS No information on uncertainties. 1484100400004 STATUS (TABLE,,W.-J.Ong+,J,PR/C,110,024321,2024) 1484100400005 page 024321-4 of J,PR/C,110,024321,2024. 1484100400006 ENDBIB 4 0 1484100400007 NOCOMMON 0 0 1484100400008 DATA 1 1 1484100400009 DATA-MAX 1484100400010 NO-DIM 1484100400011 0.01 1484100400012 ENDDATA 3 0 1484100400013 ENDSUBENT 12 0 1484100499999 ENDENTRY 4 0 1484199999999