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| /*===================================================================*/
/* NRDF D1796 Data No.2 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,2;
D#=D1796;
TITLE=/ Compressional-mode giant resonances in deformed nuclei /;
ATH=(M.ITOH'1', H.SAKAGUCHI'1', M.UCHIDA'1', T.ISHIKAWA'1',
T.KAWABATA'1', T.MURAKAMI'1', H.TAKEDA'1', T.TAKI'1',
S.TERASHIMA'1', N.TSUKAHARA'1', Y.YASUDA'1', M.YOSOI'1',
U.GARG'2', M.HEDDEN'2', B.KHARRAJA'2', M.KOSS'2', B.K.NAYAK'2',
S.ZHU'2', H.FUJIMURA'3', M.FUJIWARA'3,4', K.HARA'3',
H.P.YOSHIDA'3', H.AKIMUNE'5', M.N.HARAKEH'6', M.VOLKERTS'6');
INST-ATH=(2JPNKTO'1', 1USANOT'2', 2JPNRCN'3', 2JPNJAE'4', 2JPNKON'5',
2NEDGRN'6');
/* '1' Department of Physics */
/* '2' Physics Department */
/* '4' Advanced Science Research Center */
/* '5' Department of Physics */
/* '6' Kernfysisch Versneller Instituut (KVI) */
REF=PL/B;
VLP=549(2002)58;
RCTS=(144SM(ALPHA,ALPHA)144SM, 148SM(ALPHA,ALPHA)148SM,
150SM(ALPHA,ALPHA)150SM, 152SM(ALPHA,ALPHA)152SM,
154SM(ALPHA,ALPHA)154SM, SM(ALPHA,ALPHA)SM);
PHQS=(ENGY-SPEC, ANGL-DSTRN'7', EWSR'8', DEFM-PARA, STRGTH-FUNCT'9',
STRGTH-FUNCT'10', STRGTH-FUNCT'11', STRGTH-FUNCT'12');
/* '7' Double differential cross section with scattered alpha
particle. */
/* '8' Fitting parameters for GMR and GQR */
/* '9' S0(Ex) : The definition is shown in reference. */
/* '10' S2(Ex) : The definition is shown in reference. */
/* '11' S1(Ex) : The definition is shown in reference. */
/* '12' S3(Ex) : The definition is shown in reference. */
/*===================================================================*/
/* Experimental Conditions */
/*===================================================================*/
\\EXP,2;
/* 2003-12-19 : Compiled, Am + Ia */
RTY=INEL-SCATT;
ENR=X%;
CHM=ELM;
PHYS-FORM=SLD;
THK-TGT=2[10MG/CM**2;
BAC=SELF;
POL-TGT=0%;
ALGN-TGT=0%;
ACC=CYC'13';
/* '13' Isochronous cyclotron, AVF cyclotron and ring cyclotron
INST-ACC=2JPNRCN;
INC-ENGY-LAB=386MEV'14';
/* '14' Reference gives 400 MeV for incident energy value,
however correct value is 386 MeV (private communication with
H.Sakaguchi (2003.12.17)). */
CHRG-INC-ION=2+;
POL-PRJ=0%;
DET-PARTCL=ALPHA;
COINC=NO;
ANT-COINC=NO;
DET-SYS=(MAG'15',MWDC'16',SCT'17');
/* '15' Inelastically-scattered particles were analyzed by a
magnetic spectrometer, Grand Raiden. [M. Fujiwara et al.,
Nucl. Instrum. Methods Phys. Res. A 422 (1999) 484]. The
typical energy resolution was about 200 keV. */
/* '16' To determine vertical and horizontal positions in the
focal plane. */
/* '17' To determine vertical and horizontal positions in the
focal plane. */
/* 2007-02-13 : Altered, N.Otuka. SF7 corrected */
RCT=148SM(ALPHA,ALPHA)148SM;
PHQ=ENGY-SPEC;
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,2;
INC-ENGY-LAB=386MEV'18';
/* '18' Reference gives 400 MeV for incident energy value,
however correct value is 386 MeV (private communication with
H.Sakaguchi (2003.12.17)). */
THTL=[0.7DEG;
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
EXC-ENGY DSIGMA/DOMEGA/DE DELTA-DSIGMA/DOMEGA/DE
(MEV) (MB/SR/MEV) (MB/SR/MEV)
8.125 0.64912E+02 +-0.80568E+01
8.375 0.65339E+02 +-0.80832E+01
8.625 0.64082E+02 +-0.80051E+01
8.875 0.61361E+02 +-0.78333E+01
9.125 0.65406E+02 +-0.80874E+01
9.375 0.62639E+02 +-0.79145E+01
9.625 0.69459E+02 +-0.83342E+01
9.875 0.69085E+02 +-0.83117E+01
10.125 0.73354E+02 +-0.85647E+01
10.375 0.79755E+02 +-0.89306E+01
10.625 0.84646E+02 +-0.92003E+01
10.875 0.87509E+02 +-0.93546E+01
11.125 0.96056E+02 +-0.98008E+01
11.375 0.10166E+03 +-0.10083E+02
11.625 0.10800E+03 +-0.10392E+02
11.875 0.11159E+03 +-0.10563E+02
12.125 0.12337E+03 +-0.11107E+02
12.375 0.11815E+03 +-0.10870E+02
12.625 0.12428E+03 +-0.11148E+02
12.875 0.12471E+03 +-0.11167E+02
13.125 0.13083E+03 +-0.11438E+02
13.375 0.13653E+03 +-0.11685E+02
13.625 0.14065E+03 +-0.11860E+02
13.875 0.14397E+03 +-0.11999E+02
14.125 0.14571E+03 +-0.12071E+02
14.375 0.14663E+03 +-0.12109E+02
14.625 0.14793E+03 +-0.12163E+02
14.875 0.14651E+03 +-0.12104E+02
15.125 0.15146E+03 +-0.12307E+02
15.375 0.13649E+03 +-0.11683E+02
15.625 0.13324E+03 +-0.11543E+02
15.875 0.12307E+03 +-0.11094E+02
16.125 0.11123E+03 +-0.10546E+02
16.375 0.10135E+03 +-0.10067E+02
16.625 0.96744E+02 +-0.98359E+01
16.875 0.88227E+02 +-0.93929E+01
17.125 0.81355E+02 +-0.90197E+01
17.375 0.72607E+02 +-0.85210E+01
17.625 0.71388E+02 +-0.84491E+01
17.875 0.68075E+02 +-0.82508E+01
18.125 0.66430E+02 +-0.81505E+01
18.375 0.64980E+02 +-0.80610E+01
18.625 0.61727E+02 +-0.78566E+01
18.875 0.55648E+02 +-0.74597E+01
19.125 0.59342E+02 +-0.77033E+01
19.375 0.57390E+02 +-0.75756E+01
19.625 0.57958E+02 +-0.76130E+01
19.875 0.53532E+02 +-0.73165E+01
20.125 0.57128E+02 +-0.75583E+01
20.375 0.54997E+02 +-0.74160E+01
20.625 0.56104E+02 +-0.74902E+01
20.875 0.53090E+02 +-0.72863E+01
21.125 0.54892E+02 +-0.74089E+01
21.375 0.58257E+02 +-0.76327E+01
21.625 0.57540E+02 +-0.75855E+01
21.875 0.57151E+02 +-0.75598E+01
22.125 0.60882E+02 +-0.78027E+01
22.375 0.56074E+02 +-0.74883E+01
22.625 0.56650E+02 +-0.75266E+01
22.875 0.51565E+02 +-0.71809E+01
23.125 0.53950E+02 +-0.73451E+01
23.375 0.55207E+02 +-0.74301E+01
23.625 0.54885E+02 +-0.74084E+01
23.875 0.53075E+02 +-0.72853E+01
24.125 0.53023E+02 +-0.72817E+01
24.375 0.55446E+02 +-0.74462E+01
24.625 0.50182E+02 +-0.70839E+01
24.875 0.47019E+02 +-0.68570E+01
25.125 0.48679E+02 +-0.69770E+01
25.375 0.47931E+02 +-0.69232E+01
25.625 0.46241E+02 +-0.68001E+01
25.875 0.46428E+02 +-0.68138E+01
26.125 0.46248E+02 +-0.68006E+01
26.375 0.44297E+02 +-0.66556E+01
26.625 0.41126E+02 +-0.64130E+01
26.875 0.44745E+02 +-0.66892E+01
27.125 0.41874E+02 +-0.64710E+01
27.375 0.37201E+02 +-0.60992E+01
27.625 0.40528E+02 +-0.63662E+01
27.875 0.40244E+02 +-0.63438E+01
28.125 0.40124E+02 +-0.63344E+01
28.375 0.40177E+02 +-0.63385E+01
28.625 0.38262E+02 +-0.61857E+01
28.875 0.37896E+02 +-0.61560E+01
29.125 0.37111E+02 +-0.60919E+01
29.375 0.37567E+02 +-0.61292E+01
29.625 0.36946E+02 +-0.60784E+01
29.875 0.37395E+02 +-0.61152E+01
30.125 0.34000E+02 +-0.58310E+01
30.375 0.35600E+02 +-0.59666E+01
30.625 0.36722E+02 +-0.60599E+01
30.875 0.35399E+02 +-0.59497E+01
31.125 0.33746E+02 +-0.58091E+01
31.375 0.32251E+02 +-0.56790E+01
31.625 0.33619E+02 +-0.57982E+01
31.875 0.34733E+02 +-0.58935E+01
32.125 0.34733E+02 +-0.58935E+01
32.375 0.35219E+02 +-0.59346E+01
32.625 0.34621E+02 +-0.58840E+01
32.875 0.33783E+02 +-0.58124E+01
33.125 0.32123E+02 +-0.56678E+01
33.375 0.32766E+02 +-0.57242E+01
33.625 0.30673E+02 +-0.55383E+01
33.875 0.31585E+02 +-0.56201E+01
34.125 0.31966E+02 +-0.56539E+01
34.375 0.31017E+02 +-0.55693E+01
34.625 0.29933E+02 +-0.54711E+01
34.875 0.32086E+02 +-0.56645E+01
\END;
/*===================================================================*/
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