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| /*===================================================================*/
/* NRDF D1721 Data No.2 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,2;
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,2;
/* 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(12BE,12BE)P;
PHQ=ENGY-SPEC;
INC-ENGY-LAB=53.8MEV/A;
DET-PARTCL=(12BE,GAMMA);
COINC=(GAMMA,12BE);
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,2;
INC-ENGY-LAB=53.8MEV/A;
EMT-1=GAMMA;
THTL-1=67[148DEG;
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
ENGY-EMT COUNTS'12' DELTA-COUNTS'12'
(MEV) (ARB) (ARB)
1.128E+00 1.305E+02 +-4.298E+01
1.148E+00 1.631E+02 +-4.002E+01
1.170E+00 1.209E+02 +-3.891E+01
1.186E+00 1.676E+02 +-4.113E+01
1.207E+00 1.009E+02 +-4.002E+01
1.228E+00 1.090E+02 +-3.815E+01
1.247E+00 1.264E+02 +-3.779E+01
1.271E+00 1.603E+02 +-3.949E+01
1.291E+00 1.242E+02 +-3.891E+01
1.311E+00 2.093E+02 +-3.841E+01
1.331E+00 1.125E+02 +-3.832E+01
1.351E+00 1.902E+02 +-4.043E+01
1.371E+00 7.314E+01 +-3.897E+01
1.391E+00 1.090E+02 +-3.815E+01
1.411E+00 1.711E+02 +-3.689E+01
1.430E+00 1.042E+02 +-3.779E+01
1.452E+00 1.231E+02 +-3.557E+01
1.470E+00 1.364E+02 +-3.557E+01
1.489E+00 1.264E+02 +-3.779E+01
1.510E+00 1.431E+02 +-3.668E+01
1.531E+00 1.078E+02 +-3.695E+01
1.550E+00 1.352E+02 +-3.656E+01
1.569E+00 1.420E+02 +-3.446E+01
1.590E+00 1.866E+02 +-3.572E+01
1.612E+00 1.364E+02 +-3.446E+01
1.631E+00 2.009E+02 +-3.446E+01
1.650E+00 1.615E+02 +-3.607E+01
1.671E+00 1.287E+02 +-3.446E+01
1.693E+00 1.320E+02 +-3.335E+01
1.713E+00 1.042E+02 +-3.557E+01
1.733E+00 1.509E+02 +-3.446E+01
1.752E+00 1.109E+02 +-3.335E+01
1.773E+00 1.448E+02 +-3.171E+01
1.792E+00 1.387E+02 +-3.224E+01
1.814E+00 9.197E+01 +-3.335E+01
1.830E+00 1.878E+02 +-3.200E+01
1.851E+00 1.120E+02 +-3.224E+01
1.873E+00 1.451E+02 +-3.201E+01
1.895E+00 1.220E+02 +-3.114E+01
1.911E+00 1.497E+02 +-3.216E+01
1.934E+00 1.359E+02 +-3.059E+01
1.953E+00 1.498E+02 +-3.224E+01
1.972E+00 1.635E+02 +-3.263E+01
1.991E+00 2.153E+02 +-3.340E+01
2.014E+00 1.773E+02 +-3.309E+01
2.030E+00 2.970E+02 +-3.496E+01
2.049E+00 3.638E+02 +-3.830E+01
2.070E+00 4.499E+02 +-3.891E+01
2.091E+00 4.041E+02 +-4.091E+01
2.110E+00 3.845E+02 +-4.131E+01
2.129E+00 4.588E+02 +-3.861E+01
2.152E+00 3.339E+02 +-3.740E+01
2.174E+00 3.212E+02 +-3.693E+01
2.191E+00 2.354E+02 +-3.557E+01
2.213E+00 2.383E+02 +-3.152E+01
2.234E+00 1.742E+02 +-2.890E+01
2.254E+00 1.220E+02 +-2.781E+01
2.270E+00 7.714E+01 +-2.408E+01
2.293E+00 8.289E+01 +-2.464E+01
2.315E+00 5.065E+01 +-2.204E+01
2.333E+00 8.085E+01 +-2.223E+01
2.352E+00 4.306E+01 +-2.112E+01
2.373E+00 5.871E+01 +-2.103E+01
2.395E+00 1.727E+01 +-2.134E+01
2.414E+00 -3.030E+01 +-1.890E+01
2.429E+00 1.972E+01 +-2.001E+01
2.451E+00 1.305E+01 +-2.001E+01
2.472E+00 1.932E+00 +-1.890E+01
2.491E+00 2.750E+01 +-2.001E+01
2.513E+00 3.750E+01 +-1.890E+01
2.534E+00 4.862E+01 +-1.890E+01
2.553E+00 9.713E+00 +-2.001E+01
2.575E+00 4.862E+01 +-1.890E+01
2.593E+00 1.416E+01 +-1.890E+01
2.612E+00 3.194E+01 +-1.890E+01
2.633E+00 4.417E+01 +-1.890E+01
2.652E+00 5.084E+01 +-1.890E+01
2.670E+00 4.862E+01 +-2.001E+01
2.692E+00 3.306E+01 +-1.890E+01
2.711E+00 2.861E+01 +-1.890E+01
2.732E+00 3.083E+01 +-1.890E+01
2.754E+00 4.862E+01 +-1.890E+01
2.776E+00 1.305E+01 +-1.779E+01
2.794E+00 5.418E+01 +-1.890E+01
2.813E+00 5.195E+01 +-1.890E+01
2.834E+00 3.528E+01 +-1.779E+01
2.853E+00 3.306E+01 +-1.779E+01
2.875E+00 2.861E+01 +-1.667E+01
2.893E+00 3.083E+01 +-1.667E+01
\END;
/*===================================================================*/
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