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| /*===================================================================*/
/* NRDF D1796 Data No.5 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,5;
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,5;
/* 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=154SM(ALPHA,ALPHA)154SM;
PHQ=ENGY-SPEC;
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,5;
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 0.64987E+02 +-0.80615E+01
8.375 0.62211E+02 +-0.78874E+01
8.625 0.72779E+02 +-0.85311E+01
8.875 0.72180E+02 +-0.84959E+01
9.125 0.82149E+02 +-0.90636E+01
9.375 0.87133E+02 +-0.93345E+01
9.625 0.91550E+02 +-0.95682E+01
9.875 0.95967E+02 +-0.97963E+01
10.125 0.10269E+03 +-0.10133E+02
10.375 0.10934E+03 +-0.10457E+02
10.625 0.11149E+03 +-0.10559E+02
10.875 0.12436E+03 +-0.11152E+02
11.125 0.12830E+03 +-0.11327E+02
11.375 0.13351E+03 +-0.11555E+02
11.625 0.13770E+03 +-0.11735E+02
11.875 0.14174E+03 +-0.11906E+02
12.125 0.14427E+03 +-0.12011E+02
12.375 0.13363E+03 +-0.11560E+02
12.625 0.13695E+03 +-0.11702E+02
12.875 0.13493E+03 +-0.11616E+02
13.125 0.13414E+03 +-0.11582E+02
13.375 0.13423E+03 +-0.11586E+02
13.625 0.13004E+03 +-0.11403E+02
13.875 0.13903E+03 +-0.11791E+02
14.125 0.13370E+03 +-0.11563E+02
14.375 0.13827E+03 +-0.11759E+02
14.625 0.12950E+03 +-0.11380E+02
14.875 0.14117E+03 +-0.11882E+02
15.125 0.13764E+03 +-0.11732E+02
15.375 0.13190E+03 +-0.11485E+02
15.625 0.13247E+03 +-0.11509E+02
15.875 0.12890E+03 +-0.11353E+02
16.125 0.11978E+03 +-0.10945E+02
16.375 0.11370E+03 +-0.10663E+02
16.625 0.10619E+03 +-0.10305E+02
16.875 0.95935E+02 +-0.97946E+01
17.125 0.87638E+02 +-0.93615E+01
17.375 0.78174E+02 +-0.88416E+01
17.625 0.80130E+02 +-0.89515E+01
17.875 0.71170E+02 +-0.84363E+01
18.125 0.73379E+02 +-0.85661E+01
18.375 0.63820E+02 +-0.79887E+01
18.625 0.67069E+02 +-0.81896E+01
18.875 0.60287E+02 +-0.77645E+01
19.125 0.60823E+02 +-0.77989E+01
19.375 0.59309E+02 +-0.77012E+01
19.625 0.51801E+02 +-0.71973E+01
19.875 0.60791E+02 +-0.77969E+01
20.125 0.58015E+02 +-0.76168E+01
20.375 0.57069E+02 +-0.75544E+01
20.625 0.60224E+02 +-0.77604E+01
20.875 0.56533E+02 +-0.75188E+01
21.125 0.53883E+02 +-0.73405E+01
21.375 0.51990E+02 +-0.72104E+01
21.625 0.54009E+02 +-0.73491E+01
21.875 0.53441E+02 +-0.73103E+01
22.125 0.55681E+02 +-0.74620E+01
22.375 0.53536E+02 +-0.73168E+01
22.625 0.47731E+02 +-0.69088E+01
22.875 0.53441E+02 +-0.73103E+01
23.125 0.51958E+02 +-0.72082E+01
23.375 0.51233E+02 +-0.71577E+01
23.625 0.47699E+02 +-0.69065E+01
23.875 0.48867E+02 +-0.69905E+01
24.125 0.50633E+02 +-0.71157E+01
24.375 0.46879E+02 +-0.68468E+01
24.625 0.44040E+02 +-0.66363E+01
24.875 0.46343E+02 +-0.68076E+01
25.125 0.44040E+02 +-0.66363E+01
25.375 0.40538E+02 +-0.63670E+01
25.625 0.41737E+02 +-0.64604E+01
25.875 0.42589E+02 +-0.65260E+01
26.125 0.42589E+02 +-0.65260E+01
26.375 0.41074E+02 +-0.64089E+01
26.625 0.40822E+02 +-0.63892E+01
26.875 0.37888E+02 +-0.61553E+01
27.125 0.39245E+02 +-0.62646E+01
27.375 0.37005E+02 +-0.60832E+01
27.625 0.35901E+02 +-0.59917E+01
27.875 0.36405E+02 +-0.60337E+01
28.125 0.38866E+02 +-0.62343E+01
28.375 0.37794E+02 +-0.61476E+01
28.625 0.32084E+02 +-0.56642E+01
28.875 0.34765E+02 +-0.58962E+01
29.125 0.35522E+02 +-0.59600E+01
29.375 0.36311E+02 +-0.60258E+01
29.625 0.35017E+02 +-0.59175E+01
29.875 0.32399E+02 +-0.56920E+01
30.125 0.37951E+02 +-0.61605E+01
30.375 0.37667E+02 +-0.61374E+01
30.625 0.32778E+02 +-0.57252E+01
30.875 0.30695E+02 +-0.55403E+01
31.125 0.36847E+02 +-0.60702E+01
31.375 0.31768E+02 +-0.56363E+01
31.625 0.32052E+02 +-0.56614E+01
31.875 0.30317E+02 +-0.55061E+01
32.125 0.31011E+02 +-0.55687E+01
32.375 0.27572E+02 +-0.52509E+01
32.625 0.31610E+02 +-0.56223E+01
32.875 0.30569E+02 +-0.55289E+01
33.125 0.31358E+02 +-0.55998E+01
33.375 0.27667E+02 +-0.52599E+01
33.625 0.30727E+02 +-0.55432E+01
33.875 0.32399E+02 +-0.56920E+01
34.125 0.28519E+02 +-0.53403E+01
34.375 0.30506E+02 +-0.55232E+01
34.625 0.30412E+02 +-0.55147E+01
34.875 0.28771E+02 +-0.53639E+01
\END;
/*===================================================================*/
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