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| /*===================================================================*/
/* NRDF D1827 Data No.3 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,3;
D#=D1827;
TITLE=/ Momentum distributions of 14C and 15C fragments from 16C
breakup /;
ATH=(T.YAMAGUCHI'1', T.ZHENG'1,2,3', A.OZAWA'1', M.CHIBA'1,4',
R.KANUNGO'1', T.KATO'1', K.MORIMOTO'1', T.OHNISHI'1', T.SUDA'1',
Y.YAMAGUCHI'1,5', A.YOSHIDA'1', K.YOSHIDA'1', I.TANIHATA'1');
INST-ATH=(2JPNIPC'1', 2JPNSUT'2', 3CPRBJG'3', 2JPNTOH'4',
2JPNNII'5');
/* '2' Department of Physics */
/* '3' Department of Technical Physics */
/* '4' Department of Physics */
/* '5' Department of Physics */
REF=NP/A;
VLP=724(2003)3;
RCTS=(C(16C,15C)X, C(16C,14C)X);
PHQS=(MOM-DSTRN'6', XSECTN'7', XSECTN'8');
/* '6' longitudinal momentum distribution */
/* '7' one neutron removal cross section */
/* '8' two neutrons removal cross section */
/*===================================================================*/
/* Experimental Conditions */
/*===================================================================*/
\\EXP,3;
/* 2003-09-01 : Compiled, Km + Am */
ENR=NAT;
CHM=ELM;
PHYS-FORM=SLD;
THK-TGT=370MG/CM**2;
BAC=X;
POL-TGT=0%;
ALGN-TGT=0%;
ACC=PRJFS'9';
/* '9' Primary beam, 22Ne of 110 AMeV, was used to bombard a Be
target to produce a 16C secondary beam through the projectile
fragmentation reaction. */
INST-ACC=2JPNIPC;
INC-ENGY-LAB=83MEV/A'10';
/* '10' Around 83 MeV/A at the middle of the carbon target. */
ERS-PRJ=XKEV'11';
/* '11' The momentum broadening was confined to +-0.4 percent by
a momentum slit. */
POL-PRJ=0%;
COINC=NO;
ANT-COINC=NO;
DET-SYS=(MAG,SCT'12',NAI'13',SI'14',TOF'15',EDE'16');
/* '12' To obtain ToF signal */
/* '13' NaI(Tl) detector to measure total energy */
/* '14' To identify charge of fragment */
/* '15' To obtain fragment velocity */
/* '16' To identify particles */
CALB-DET=/ TOF was calibrated by using the primary beam with several
energies obtained by passing through different thicknesses
of Be (2, 4, 7.5, 9 mm). /;
/* Experimental Method:
- Time-of-flight (To obtain fragment velocity)
- Particle identification by 'E/Delta E' measurement (To identify
particles)
RCT=C(16C,15C)X;
RTY=INCL;
PHQ=XSECTN'24';
/* '24' one neutron removal cross section */
DET-PARTCL=15C;
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,3;
INC-ENGY-LAB=83MEV/A'17';
/* '17' Around 83 MeV/A at the middle of the carbon target. */
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
XSECTN'25' DELTA-XSECTN'25'
(MB) (MB)
65 +15-10
\END;
/*===================================================================*/
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