ENTRY S0228 20201225 S029S022800000001 SUBENT S0228001 20201225 S029S022800100001 BIB 10 53 S022800100002 TITLE Quadrupole deformation of 16C studied by proton and S022800100003 deuteron inelastic scattering S022800100004 AUTHOR (Y.Jiang,J.L.Lou,Y.L.Ye,Y.Liu,Z.W.Tan,W.Liu,B.Yang, S022800100005 L.C.Tao,K.Ma,Z.H.Li,Q.T.Li,X.F.Yang,J.Y.Xu,H.Z.Yu, S022800100006 J.X.Han,S.W.Bai,S.W.Huang,G.Li,H.Y.Wu,H.L.Zang, S022800100007 J.Feng,Z.Q.Chen,Y.D.Chen,Q.Yuan,J.G.Li,B.S.Hu,F.R.Xu, S022800100008 J.S.Wang,Y.Y.Yang,P.Ma,Q.Hu,Z.Bai,Z.H.Gao,F.F.Duan, S022800100009 L.Y.Hu,J.H.Tan,S.Q.Sun,Y.S.Song,H.J.Ong,D.T.Tran, S022800100010 D.Y.Pang,C.X.Yuan) S022800100011 INSTITUTE (3CPRBJG,3CPRIMP,2JPNOSA,3CPRBHN,3CPRSZH) S022800100012 (3CPRCPR) Harbin Engineering University, Harbin S022800100013 REFERENCE (J,PR/C,101,024601,2020) S022800100014 #doi:10.1103/PhysRevC.101.024601 S022800100015 FACILITY (CYCLO,3CPRIMP) Radioactive Ion Beam Line S022800100016 in Lanzhou (RIBLL) S022800100017 INC-SOURCE (FRAGM) A 16C secondary beam at about 24.0 S022800100018 MeV/nucleon was produced from a 18O primary beam at S022800100019 59.6MeV/nucleon impinging on a 9Be target with a S022800100020 thickness of 4.5 mm. The average beam intensity and S022800100021 the purity of 16C were up to 1E4 particles per second S022800100022 and 90%, respectively. S022800100023 METHOD (COINC) Detection of outgoing 16C and recoil S022800100024 protons/deuterons in coincidence. S022800100025 (EDEG,TOF,EDE) The secondary beam was purified by a S022800100026 uniform 650-um aluminum degrader, and was identified S022800100027 by the time-of-flight and energy losses. The charged S022800100028 particles were detected and identified with standard S022800100029 Delta E-E methods. S022800100030 SAMPLE A 4.37 +- 0.05 mg/cm2 (CH2)n target was used to S022800100031 measure the protons scattering data. S022800100032 A 9.53 +- 0.12 mg/cm2 (CD2)n target were used to S022800100033 measure the deuterons scattering data. S022800100034 A 13.73 +-0.13 mg/cm2 carbon target was employed to S022800100035 subtract the background coming from carbon atoms in S022800100036 the (CH2)n and (CD2)n targets. S022800100037 DETECTOR (PPAC) Three PPACs were installed upstream of targets S022800100038 to provide beam tracking information, with a S022800100039 resolution of the hit position on the target less S022800100040 than 1.0 mm. S022800100041 (TELES,SISD,SI,CSICR) A set of double-sided annular S022800100042 silicon strip detector (DSSD) and five telescopes (T0, S022800100043 T1UP, T1DOWN, T2UP, T2DOWN) were used to detect S022800100044 and identify the charged particles. T0 and T2 were S022800100045 employed to detect the elastic and inelastic S022800100046 scattering channels. The telescope T0 consists of S022800100047 three 1000-um-thick DSSDs, three 1500-um-thick S022800100048 large-surface silicon detectors (SSDs), and a layer of S022800100049 4-cm-thick CsI(Tl) crystals. The telescope T2 was S022800100050 composed of a 300-um-thick DSSD, a 1500-um-thick SSD, S022800100051 and a layer of CsI(Tl) crystals. other telescopes were S022800100052 employed to detect transfer reaction channels. S022800100053 HISTORY (20201225C) Jimin Wang (CNDC) S022800100054 (20201225R) Data received from J.L.Lou S022800100055 ENDBIB 53 0 S022800100056 COMMON 1 3 S022800100057 EN S022800100058 MEV/A S022800100059 24.0 S022800100060 ENDCOMMON 3 0 S022800100061 ENDSUBENT 60 0 S022800199999 SUBENT S0228002 20201225 S029S022800200001 BIB 3 14 S022800200002 REACTION ((1-H-1(6-C-16,EL)1-H-1,,DA,,RTH)= S022800200003 (6-C-16(P,EL)6-C-16,,DA,,RTH)) S022800200004 ERR-ANALYS (ERR-S) Statistical errors including the errors from S022800200005 the numbers of elastically scattered protons and the S022800200006 incoming 16C, as well as from the subtraction of the S022800200007 carbon background. S022800200008 (ERR-SYS,,10.) The systematical errors were estimated S022800200009 to be less than 10%, taking into account the S022800200010 uncertainties in geometrical efficiency determination, S022800200011 the thickness of the target, the particle S022800200012 identification gate of 16C, and the cuts applied on S022800200013 the Q-value spectra. S022800200014 STATUS (TABLE) Fig.7 (a) of Phys. Rev. C 101,024601(2020) S022800200015 Data were obtained from AUTHOR S022800200016 ENDBIB 14 0 S022800200017 NOCOMMON 0 0 S022800200018 DATA 3 9 S022800200019 ANG-CM DATA ERR-S S022800200020 ADEG NO-DIM NO-DIM S022800200021 50.99 6.34 1.09 S022800200022 47.07 4.88 0.80 S022800200023 43.16 4.44 0.68 S022800200024 39.20 7.43 0.95 S022800200025 35.24 10.25 0.94 S022800200026 31.32 12.24 0.92 S022800200027 27.41 11.51 0.80 S022800200028 23.46 9.64 0.63 S022800200029 19.52 5.98 0.39 S022800200030 ENDDATA 11 0 S022800200031 ENDSUBENT 30 0 S022800299999 SUBENT S0228003 20201225 S029S022800300001 BIB 3 14 S022800300002 REACTION ((1-H-2(6-C-16,EL)1-H-2,,DA,,RTH)= S022800300003 (6-C-16(D,EL)6-C-16,,DA,,RTH)) S022800300004 ERR-ANALYS (ERR-S) Statistical errors including the errors from S022800300005 the numbers of elastically scattered deuterons and S022800300006 the incoming 16C, as well as from the subtraction of S022800300007 the carbon background. S022800300008 (ERR-SYS,,10.) The systematical errors were estimated S022800300009 to be less than 10%, taking into account the S022800300010 uncertainties in geometrical efficiency determination, S022800300011 the thickness of the target, the particle S022800300012 identification gate of 16C, and the cuts applied on S022800300013 the Q-value spectra. S022800300014 STATUS (TABLE) Fig.7 (b) of Phys. Rev. C 101,024601(2020) S022800300015 Data were obtained from AUTHOR S022800300016 ENDBIB 14 0 S022800300017 NOCOMMON 0 0 S022800300018 DATA 3 9 S022800300019 ANG-CM DATA ERR-S S022800300020 ADEG NO-DIM NO-DIM S022800300021 51.08 17.52 1.77 S022800300022 47.12 20.80 1.96 S022800300023 43.20 17.79 1.65 S022800300024 39.29 14.47 1.34 S022800300025 35.33 15.39 1.34 S022800300026 31.37 19.11 1.57 S022800300027 27.45 14.75 1.20 S022800300028 23.54 6.34 0.53 S022800300029 19.62 1.12 0.12 S022800300030 ENDDATA 11 0 S022800300031 ENDSUBENT 30 0 S022800399999 SUBENT S0228004 20201225 S029S022800400001 BIB 4 8 S022800400002 REACTION ((1-H-1(6-C-16,INL)1-H-1,PAR,DA)= S022800400003 (6-C-16(P,INL)6-C-16,PAR,DA)) S022800400004 EN-SEC (E-LVL,6-C-16) S022800400005 ERR-ANALYS (ERR-S) Statistical errors S022800400006 (ERR-SYS) Systematic errors were estimated to be S022800400007 about 12% S022800400008 STATUS (TABLE) Fig.8 (a) of Phys. Rev. C 101,024601(2020) S022800400009 Data were obtained from AUTHOR S022800400010 ENDBIB 8 0 S022800400011 COMMON 2 3 S022800400012 E-LVL ERR-SYS S022800400013 MEV PER-CENT S022800400014 1.766 12.0 S022800400015 ENDCOMMON 3 0 S022800400016 DATA 3 3 S022800400017 ANG-CM DATA-CM ERR-S S022800400018 ADEG MB/SR MB/SR S022800400019 43.46 3.59 1.07 S022800400020 35.26 8.14 1.80 S022800400021 27.14 9.25 1.94 S022800400022 ENDDATA 5 0 S022800400023 ENDSUBENT 22 0 S022800499999 SUBENT S0228005 20201225 S029S022800500001 BIB 4 8 S022800500002 REACTION ((1-H-2(6-C-16,INL)1-H-2,PAR,DA)= S022800500003 (6-C-16(D,INL)6-C-16,PAR,DA)) S022800500004 EN-SEC (E-LVL,6-C-16) S022800500005 ERR-ANALYS (ERR-S) Statistical errors S022800500006 (ERR-SYS) Systematic errors were estimated to be S022800500007 about 12% S022800500008 STATUS (TABLE) Fig.8 (b) of Phys. Rev. C 101,024601(2020) S022800500009 Data were obtained from AUTHOR S022800500010 ENDBIB 8 0 S022800500011 COMMON 2 3 S022800500012 E-LVL ERR-SYS S022800500013 MEV PER-CENT S022800500014 1.766 12.0 S022800500015 ENDCOMMON 3 0 S022800500016 DATA 3 6 S022800500017 ANG-CM DATA-CM ERR-S S022800500018 ADEG MB/SR MB/SR S022800500019 54.78 1.69 0.30 S022800500020 50.70 3.43 0.44 S022800500021 46.24 5.26 0.56 S022800500022 41.92 5.96 0.62 S022800500023 37.65 6.56 0.70 S022800500024 33.33 7.70 0.78 S022800500025 ENDDATA 8 0 S022800500026 ENDSUBENT 25 0 S022800599999 ENDENTRY 5 0 S022899999999