ENTRY S0188 20200218 S027S018800000001 SUBENT S0188001 20200218 S027S018800100001 BIB 13 44 S018800100002 TITLE Two-neutron removal cross sections from 15,16C at S018800100003 around 240 MeV/nucleon S018800100004 AUTHOR (Y.Z.Sun,S.T.Wang,Z.Y.Sun,X.H.Zhang,D.Yan,B.H.Sun, S018800100005 J.W.Zhao,Y.P.Xu,D.Y.Pang,Y.H.Yu,K.Yue,S.W.Tang, S018800100006 C.Dong,Y.X.Zhao,F.Fang,Y.Sun,Z.H.Cheng,X.M.Liu,P.Ma, S018800100007 H.R.Yang,C.G.Lu,L.M.Duan) S018800100008 INSTITUTE (3CPRIMP,3CPRUCA,3CPRBHN,3CPRLNZ) S018800100009 REFERENCE (J,PR/C,99,024605,2019) S018800100010 #doi:10.1103/PhysRevC.99.024605 S018800100011 FACILITY (CYCLO,3CPRIMP) Heavy ion research facility (HIRFL) S018800100012 INC-SOURCE Primary beam of O-18 was extracted and accelerated to S018800100013 280 MeV/nucleon by the main Cooler Storage Ring (CSRm),S018800100014 and directed onto a beryllium target of 15 mm S018800100015 thickness. The reaction products from projectile S018800100016 fragmentation of O-18 were separated according to S018800100017 their magnetic rigidity using the in-flight fragment S018800100018 separator Second Radioactive Ion Beam Line (RIBLL2). S018800100019 SAMPLE A 900 mg/cm2 thick carbon reaction target S018800100020 DETECTOR (SCIN,IOCH) The secondary beams were identified based S018800100021 on a combination of the time of flight from SC1 to S018800100022 SC2 measured between two plastic scintillator S018800100023 detectors (SC1 and SC2) and the energy loss measured S018800100024 with a multiple sampling ionization chamber (MUSIC1). S018800100025 (SCIN) The time of flight from SC2 to TOFW was S018800100026 measured between a plastic scintillator (SC2) and a S018800100027 plastic scintillator wall (TOFW) with 30 strips and S018800100028 an active area of 120 x 120 cm2 placed about 10 m S018800100029 downstream from the target. The time of flight was S018800100030 calibrated using the O-18 primary beam, and a S018800100031 resolution of about 300 ps. S018800100032 (IOCH) The energy loss was measured by a multiple S018800100033 sampling ionization chamber (MUSIC2) placed 50 cm S018800100034 downstream of the reaction target. S018800100035 METHOD (TOF) S018800100036 CORRECTION The background contributions were measured by using S018800100037 target-out runs and subtracted. S018800100038 ERR-ANALYS (ERR-T) The total uncertainty in the cross sections S018800100039 mainly comes from statistical error. S018800100040 (ERR-1) The uncertainty arising from the software S018800100041 gates used for particle identification and the S018800100042 transmission efficiency is estimated to be 5%. S018800100043 STATUS (TABLE) Data taken from the text of S018800100044 Phys.Rev.C,99,024605 (2019) S018800100045 HISTORY (20200218C) Jimin Wang (CNDC). S018800100046 ENDBIB 44 0 S018800100047 COMMON 2 3 S018800100048 EN ERR-1 S018800100049 MEV/A PER-CENT S018800100050 240. 5. S018800100051 ENDCOMMON 3 0 S018800100052 ENDSUBENT 51 0 S018800199999 SUBENT S0188002 20200218 S027S018800200001 BIB 1 1 S018800200002 REACTION (6-C-15(8-O-18,X)6-C-13,,SIG) S018800200003 ENDBIB 1 0 S018800200004 NOCOMMON 0 0 S018800200005 DATA 2 1 S018800200006 DATA ERR-T S018800200007 MB MB S018800200008 64. 10. S018800200009 ENDDATA 3 0 S018800200010 ENDSUBENT 9 0 S018800299999 SUBENT S0188003 20200218 S027S018800300001 BIB 1 1 S018800300002 REACTION (6-C-16(8-O-18,X)6-C-14,,SIG) S018800300003 ENDBIB 1 0 S018800300004 NOCOMMON 0 0 S018800300005 DATA 2 1 S018800300006 DATA ERR-T S018800300007 MB MB S018800300008 97. 13. S018800300009 ENDDATA 3 0 S018800300010 ENDSUBENT 9 0 S018800399999 ENDENTRY 3 0 S018899999999