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| /*===================================================================*/
/* NRDF D1721 Data No.1 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,1;
D#=D1721;
TITLE=/ Quadrupole deformation of 12Be studied by proton inelastic
scattering /;
ATH=(H.IWASAKI'1', T.MOTOBAYASHI'2', H.AKIYOSHI'3', Y.ANDO'2',
N.FUKUDA'1', H.FUJIWARA'2', ZS.FULOP'3', K.I.HAHN'3',
Y.HIGURASHI'2', M.HIRAI'1', I.HISANAGA'2', N.IWASA'3',
T.KIJIMA'2', T.MINEMURA'2', T.NAKAMURA'1', M.NOTANI'3',
S.OZAWA'2', H.SAKURAI'3', S.SHIMOURA'2', S.TAKEUCHI'2',
T.TERANISHI'3', Y.YANAGISAWA'2', M.ISHIHARA'1,3');
INST-ATH=(2JPNTOK'1', 2JPNRIK'2', 2JPNIPC'3');
/* '1' Department of Physics */
/* '2' Department of Physics */
REF=PL/B;
VLP=481(2000)7;
RCTS=(P(10BE,10BE)P, P(12BE,12BE)P);
PHQS=(ENGY-SPEC, XSECTN, ANGL-DSTRN, DEFM-PARA);
/*===================================================================*/
/* Experimental Conditions */
/*===================================================================*/
\\EXP,1;
/* 2002-09-05 : Converted, Ay + On. Data converted to EXFOR E1721
/* 2003-06-25 : Altered, On. REACTION corrected */
RTY=INEL-SCATT;
ENR=X%;
CHM=X'4';
/* '4' CH2 and C are used */
PHYS-FORM=SLD;
THK-TGT=XMG/CM**2'5';
/* '5' 90.2mg/cm2 89.8mg/cm2 for (CH2)n and C target,
respectively. */
BAC=X;
POL-TGT=0%;
ALGN-TGT=0%;
ACC=PRJFS'6';
/* '6' Secondary beams of 10Be and 12Be were produced and
separated by the RIKEN Projectile Fragment Separator [T.Kubo et
al., Nucl.Instrum.Methods B70(1992)309] using a 100MeV/u 18O
primary beam incident on a 1.11g/cm2 9Be target. */
INST-ACC=2JPNIPC;
ERS-PRJ=1%'7';
/* '7' angular spreads were limited to +-1.7deg */
POL-PRJ=0%;
ANT-COINC=NO;
DET-SYS=(SCT'8',NAI'9',TOF,EDE);
/* '8' To detect outgoing particles */
/* '9' To detect de-excitation gamma-rays */
ERS-DET=7.0%'10';
/* '10' for 1275-keV gamma-ray detection by NaI counter */
EFCN-DET=/ 83+-4(80+-4)% for the 10Be(12Be) scattering at plastic
scintillator hodoscope, 4.6(7.1)% for 3.37(2.10)MeV
gamma-ray emitted from 10Be(12Be) in flight for NaI
scintillators /;
/* Experimental Method:
- Time-of-flight
- Particle identification by 'E/Delta E' measurement
/* 2005-08-12 : Altered, On. REACTION corrected (CP-D/430) */
/* 2006-08-01 : Altered, At. Re-digitized */
RCT=P(10BE,10BE)P;
PHQ=ENGY-SPEC;
INC-ENGY-LAB=59.2MEV/A;
DET-PARTCL=(10BE,GAMMA);
COINC=(GAMMA,10BE);
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,1;
INC-ENGY-LAB=59.2MEV/A;
EMT-1=GAMMA;
THTL-1=67[148DEG;
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
ENGY-EMT COUNTS'11' DELTA-COUNTS'11'
(MEV) (ARB) (ARB)
2.127E+00 1.407E+02 +-2.854E+01
2.151E+00 1.600E+02 +-2.704E+01
2.171E+00 1.084E+02 +-2.704E+01
2.188E+00 1.306E+02 +-2.704E+01
2.210E+00 1.701E+02 +-2.684E+01
2.228E+00 1.458E+02 +-2.779E+01
2.249E+00 1.586E+02 +-2.729E+01
2.271E+00 1.588E+02 +-2.581E+01
2.292E+00 1.138E+02 +-2.627E+01
2.310E+00 1.598E+02 +-2.601E+01
2.330E+00 1.342E+02 +-2.704E+01
2.350E+00 1.576E+02 +-2.826E+01
2.367E+00 1.343E+02 +-2.701E+01
2.392E+00 1.483E+02 +-2.646E+01
2.409E+00 1.158E+02 +-2.581E+01
2.430E+00 1.281E+02 +-2.581E+01
2.447E+00 1.453E+02 +-2.581E+01
2.468E+00 1.551E+02 +-NEGLIGIBLE
2.485E+00 1.723E+02 +-2.704E+01
2.509E+00 1.809E+02 +-2.704E+01
2.530E+00 2.264E+02 +-2.826E+01
2.547E+00 1.797E+02 +-2.704E+01
2.571E+00 1.551E+02 +-2.826E+01
2.592E+00 2.018E+02 +-2.704E+01
2.612E+00 2.178E+02 +-2.704E+01
2.629E+00 1.674E+02 +-2.704E+01
2.650E+00 1.945E+02 +-2.704E+01
2.671E+00 1.613E+02 +-2.704E+01
2.692E+00 1.871E+02 +-2.704E+01
2.709E+00 1.994E+02 +-2.704E+01
2.729E+00 2.043E+02 +-2.704E+01
2.747E+00 1.797E+02 +-2.704E+01
2.771E+00 1.822E+02 +-2.826E+01
2.788E+00 2.203E+02 +-2.826E+01
2.812E+00 1.330E+02 +-2.826E+01
2.829E+00 2.006E+02 +-2.704E+01
2.850E+00 1.760E+02 +-2.826E+01
2.871E+00 1.723E+02 +-2.826E+01
2.891E+00 1.441E+02 +-2.826E+01
2.909E+00 1.822E+02 +-2.704E+01
2.929E+00 1.797E+02 +-2.581E+01
2.950E+00 2.264E+02 +-2.704E+01
2.971E+00 1.773E+02 +-2.704E+01
2.988E+00 2.006E+02 +-2.704E+01
3.012E+00 1.994E+02 +-2.581E+01
3.026E+00 1.490E+02 +-2.704E+01
3.050E+00 1.773E+02 +-2.581E+01
3.071E+00 1.613E+02 +-2.704E+01
3.091E+00 1.416E+02 +-2.581E+01
3.108E+00 2.031E+02 +-2.704E+01
3.129E+00 9.983E+01 +-2.704E+01
3.150E+00 2.055E+02 +-2.704E+01
3.170E+00 2.006E+02 +-2.704E+01
3.188E+00 1.871E+02 +-2.704E+01
3.212E+00 1.969E+02 +-2.704E+01
3.229E+00 2.510E+02 +-2.826E+01
3.250E+00 2.510E+02 +-3.072E+01
3.267E+00 2.608E+02 +-3.072E+01
3.288E+00 2.756E+02 +-3.318E+01
3.308E+00 3.087E+02 +-3.195E+01
3.329E+00 2.706E+02 +-3.318E+01
3.350E+00 3.161E+02 +-3.195E+01
3.367E+00 2.596E+02 +-3.318E+01
3.384E+00 3.296E+02 +-3.195E+01
3.405E+00 2.780E+02 +-3.195E+01
3.425E+00 2.768E+02 +-3.195E+01
3.443E+00 2.412E+02 +-2.949E+01
3.470E+00 1.932E+02 +-2.826E+01
3.487E+00 1.785E+02 +-2.704E+01
3.508E+00 1.908E+02 +-2.581E+01
3.529E+00 1.576E+02 +-2.458E+01
3.549E+00 8.877E+01 +-2.335E+01
3.570E+00 5.436E+01 +-2.089E+01
3.591E+00 6.419E+01 +-2.089E+01
3.611E+00 3.962E+01 +-2.089E+01
3.629E+00 7.525E+01 +-1.966E+01
3.649E+00 7.280E+01 +-1.966E+01
3.670E+00 -1.077E+01 +-1.720E+01
3.691E+00 2.487E+01 +-1.720E+01
3.708E+00 6.436E+00 +-NEGLIGIBLE
3.729E+00 1.135E+01 +-1.598E+01
3.749E+00 3.962E+01 +-1.720E+01
3.770E+00 6.436E+00 +-1.475E+01
3.791E+00 1.012E+01 +-1.720E+01
3.808E+00 -3.395E+00 +-1.598E+01
3.829E+00 -4.624E+00 +-1.598E+01
3.853E+00 1.012E+01 +-1.598E+01
3.870E+00 1.258E+01 +-1.598E+01
3.891E+00 1.135E+01 +-1.475E+01
\END;
/*===================================================================*/
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