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