/*===================================================================*/
 /* NRDF D1796 Data No.16                                             */
 /*===================================================================*/
 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,16;
 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,16;
 /* 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. */
 /* 2006-09-08 : Altered, Mt. Re-digitized */
 RCT=144SM(ALPHA,ALPHA)144SM;
 PHQ=STRGTH-FUNCT'41';
 /* '41' S0(Ex) : The definition is shown in reference. */
 /* Analysis:
    - multipole-decomposition (MD) analysis. [B. Bonin et al., Nucl.
      Phys. A 430 (1984) 349]
    - Breit-Wigner fits
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,16;
 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)). */
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 EXC-ENGY STRGTH-FUNCT'42' DELTA-STRGTH-FUNCT'42'
 (MEV) (UNIT) (UNIT)
 9.886E+00 124.6 +-42.4
 1.083E+01 246.5 +-68.9
 1.172E+01 273 +-116.6
 1.267E+01 471.7 +-116.6
 1.356E+01 885.1 +-127.2
 1.447E+01 1492 +-114
 1.540E+01 2337 +-129.9
 1.632E+01 2806 +-106
 1.727E+01 1953 +-90.1
 1.817E+01 1216 +-47.7
 1.911E+01 954 +-63.6
 2.004E+01 853.3 +-71.55
 2.096E+01 808.3 +-58.3
 2.189E+01 816.2 +-63.6
 2.278E+01 972.6 +-63.6
 2.373E+01 956.7 +-84.8
 2.467E+01 898.4 +-63.6
 2.557E+01 871.9 +-76.85
 2.650E+01 938.1 +-60.95
 2.741E+01 909 +-87.45
 2.834E+01 832.1 +-79.5
 2.926E+01 885.1 +-76.85
 3.019E+01 784.4 +-132.5
 3.110E+01 1012 +-103.4
 3.203E+01 969.9 +-132.5
 \END;
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