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/* NRDF D1796 Data No.15 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,15;
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,15;
/* 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. */
RCT=204PB(P,T)202PB;
CHM=ELM'74';
/* '74' Prepared by centrifugal settling of PbO */
PHYS-FORM=SLD;
THK-TGT=2MG/CM**2;
BAC=MYLAR;
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,15;
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)). */
INC-ENGY-LAB=51.9MEV;
SYS-ERR=<20%'75';
/* '75' Error of the absolute cross section of the ground state
transition is estimated to be less than 20%, where the main
part comes from the uncertainty of the solid angle of each
counter on the focal plane of the magnetic spectrograph. */
EMT=T;
RSD=202PB;
EXC-ENGY=0.95MEV;
J-PTY=2+;
DELTA-THTC=0.25DEG'76';
/* '76' Data-point reader uncertainty */
DELTA-DSIGMA/DOMEGA=1.9%'77';
/* '77' Data-point reader uncertainty */
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
THTC DSIGMA/DOMEGA
(DEG) (UB/SR)
4.38 118.2
6.01 126.6
8.18 117.
10.53 106.7
13.24 85.
15.41 77.5
17.94 73.6
20.1 58.6
23. 36.1
25.35 25.8
28.06 19.
30.95 21.5
33.11 23.3
35.47 21.9
38. 14.8
43.06 10.18
47.94 10.23
\END;
/*===================================================================*/
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