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| /*===================================================================*/
/* NRDF D1735 Data No.2 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,2;
D#=D1735;
TITLE=/ Soft dipole resonance in the neutron-skin nucleus 6He /;
PURPOSE=/ To measure a dipole strength at excitation energies lower
than the giant dipole resonance or spin dipole resonance in
6he /;
ATH=(S.NAKAYAMA'1', T.YAMAGATA'2', H.AKIMUNE'2', I.DAITO'3',
H.FUJIMURA'3', Y.FUJITA'4', M.FUJIWARA'3,5', K.FUSHIMI'1',
T.INOMATA'3', H.KOHRI'4', N.KOORI'1', K.TAKAHISA'3', A.TAMII'6',
M.TANAKA'7', H.TOYOKAWA'8');
INST-ATH=(2JPNTKS'1', 2JPNKON'2', 2JPNRCN'3', 2JPNOSA'4', 2JPNJAE'5',
2JPNTOK'6', 2JPNKTJ'7', 2JPNJSR'8');
/* '1' Department of Physics */
/* '2' Department of Physics */
/* '4' Department of Physics */
/* '5' Advanced Science Research Center */
/* '6' Department of Physics */
REF=PRL;
VLP=85(2000)262;
RCTS=6LI(7LI,7BE)6HE;
PHQS=(ENGY-SPEC'9', ENGY-SPEC'10', ANGL-DSTRN, RESN-WDTH,
XSECTN'11');
/* '9' Excitation energy spectrum of the residual nuclei 6He, Spin
transfer is 1. */
/* '10' Excitation energy spectrum of the residual nuclei 6He. Spin
transfer is 1. */
/* '11' at 0 deg. */
/*===================================================================*/
/* Experimental Conditions */
/*===================================================================*/
\\EXP,2;
/* 2001-10-20 : Compiled, Sr + On. */
/* 2001-11-09 : Altered, On. ANG-ERR is added to subentry E1735002
and subentry E1735003. */
/* 2001-12-17 : Altered, On. Emitted and residual particle of
reaction are corrected. */
RTY=RRG-RCT;
ENR=96.5%;
CHM=ELM;
PHYS-FORM=SLD;
THK-TGT=2.5MG/CM**2;
BAC=SELF;
POL-TGT=0%;
ALGN-TGT=0%;
ACC=CYC;
INST-ACC=2JPNRCN;
INC-ENGY-LAB=65MEV/A;
CHRG-INC-ION=+3;
POL-PRJ=0%;
DET-PARTCL=7BE;
COINC=GAMMA;
ANT-COINC=NO;
DET-SYS=(MAG'12',SCT'13');
/* '12' Grand Raiden, See M.Fujiwara et al., Nucl. Instrum.
Methods Phys. Res., Sect., A422, 484 (1999) */
/* '13' NYMPHS, GSO(Gd2SiO5:Ce) Scintillator, See S.Nakayama et
al., Nucl. Instrum. Methods Phys. Res., Sect., A404, 34 (1998)
SOLID-ANGL=XMSR'14';
/* '14' +-20mrad horizontally and +-15mrad vertically for Grand
Raiden which is set at theta(lab) of 0.3deg */
ERS-DET=500KEV'15';
/* '15' GRAND Raiden */
CALB-DET=/ A peak due to hydrogen contamination in the target is used
for the relative contribution of the Delta-S=0 and
Delta-S=1 spectra. /;
/* 2006-08-24 : Altered, At. Re-digitized */
RCT=6LI(7LI,7BE)6HE;
PHQ=ENGY-SPEC'19';
/* '19' Excitation energy spectrum of the residual nuclei 6He.
Spin transfer is 1. */
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,2;
INC-ENGY-LAB=65MEV/A;
THTL=0.75DEG;
DELTA-THTL=0.75DEG;
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
EXC-ENGY COUNTS'20' DELTA-COUNTS'20,21'
(MEV) (UNIT) (UNIT)
-5.802E+00 -1.704E-01 +-NEGLIGIBLE
-5.591E+00 1.024E+00 +-NEGLIGIBLE
-5.381E+00 1.024E+00 +-NEGLIGIBLE
-5.140E+00 1.024E+00 +-NEGLIGIBLE
-4.900E+00 1.024E+00 +-NEGLIGIBLE
-4.479E+00 1.024E+00 +-NEGLIGIBLE
-4.028E+00 3.413E+00 +-NEGLIGIBLE
-3.818E+00 4.608E+00 +-NEGLIGIBLE
-3.607E+00 8.191E+00 +-NEGLIGIBLE
-3.186E+00 3.235E+02 +-3.106E+01
-1.431E+00 3.869E+02 +-5.614E+01
-1.202E+00 2.853E+02 +-4.539E+01
-9.920E-01 2.113E+02 +-3.703E+01
-7.685E-01 7.986E+01 +-2.986E+01
-5.411E-01 1.416E+01 +-3.345E+01
-1.065E-01 1.536E+01 +-1.003E+02
5.411E-01 1.024E+00 +-8.601E+01
9.920E-01 2.133E+01 +-4.061E+01
1.202E+00 7.270E+01 +-2.747E+01
1.413E+00 3.925E+01 +-2.509E+01
1.623E+00 9.778E+01 +-2.628E+01
1.834E+00 9.061E+01 +-3.225E+01
2.074E+00 4.522E+01 +-3.225E+01
2.285E+00 3.686E+01 +-3.464E+01
2.495E+00 9.420E+01 +-3.345E+01
2.735E+00 4.403E+01 +-3.106E+01
2.946E+00 6.911E+01 +-NEGLIGIBLE
3.156E+00 9.778E+01 +-2.986E+01
3.367E+00 2.850E+01 +-3.106E+01
3.577E+00 1.061E+02 +-3.106E+01
3.818E+00 1.061E+02 +-3.225E+01
4.028E+00 1.468E+02 +-3.345E+01
4.238E+00 1.754E+02 +-3.225E+01
4.449E+00 1.265E+02 +-3.225E+01
4.659E+00 1.372E+02 +-3.345E+01
4.870E+00 1.515E+02 +-3.345E+01
5.110E+00 1.145E+02 +-3.345E+01
5.321E+00 1.420E+02 +-3.345E+01
5.531E+00 1.635E+02 +-3.345E+01
5.741E+00 1.850E+02 +-3.106E+01
5.982E+00 1.898E+02 +-3.106E+01
6.192E+00 1.957E+02 +-3.225E+01
6.403E+00 1.551E+02 +-3.106E+01
6.643E+00 1.898E+02 +-3.225E+01
6.824E+00 2.160E+02 +-3.106E+01
7.064E+00 1.695E+02 +-3.225E+01
7.244E+00 1.420E+02 +-3.225E+01
7.485E+00 1.921E+02 +-3.106E+01
7.665E+00 1.826E+02 +-3.225E+01
7.936E+00 2.196E+02 +-3.106E+01
8.086E+00 2.196E+02 +-2.867E+01
8.327E+00 2.148E+02 +-2.867E+01
8.537E+00 1.886E+02 +-2.986E+01
8.808E+00 2.280E+02 +-2.747E+01
8.988E+00 1.886E+02 +-2.867E+01
9.198E+00 2.053E+02 +-2.747E+01
9.439E+00 1.730E+02 +-2.986E+01
9.649E+00 1.503E+02 +-2.986E+01
9.860E+00 2.148E+02 +-2.867E+01
1.007E+01 1.742E+02 +-2.867E+01
1.028E+01 2.053E+02 +-2.747E+01
1.052E+01 1.503E+02 +-2.986E+01
1.073E+01 1.910E+02 +-2.867E+01
1.094E+01 1.611E+02 +-2.986E+01
1.115E+01 1.587E+02 +-2.867E+01
1.136E+01 1.599E+02 +-2.867E+01
1.160E+01 2.101E+02 +-2.628E+01
1.181E+01 1.671E+02 +-NEGLIGIBLE
1.202E+01 1.874E+02 +-2.628E+01
1.226E+01 1.802E+02 +-2.628E+01
1.251E+01 1.360E+02 +-2.747E+01
1.269E+01 1.659E+02 +-2.628E+01
1.290E+01 1.348E+02 +-2.867E+01
1.314E+01 1.659E+02 +-2.628E+01
1.335E+01 1.742E+02 +-2.628E+01
1.359E+01 1.420E+02 +-2.628E+01
1.377E+01 1.754E+02 +-2.509E+01
1.401E+01 1.456E+02 +-2.747E+01
1.422E+01 1.742E+02 +-2.509E+01
1.443E+01 1.635E+02 +-2.628E+01
1.464E+01 1.539E+02 +-2.747E+01
1.485E+01 2.005E+02 +-2.509E+01
\END;
/*===================================================================*/
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