/*===================================================================*/
 /* NRDF D1796 Data No.23                                             */
 /*===================================================================*/
 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,23;
 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,23;
 /* 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=154SM(ALPHA,ALPHA)154SM;
 PHQ=STRGTH-FUNCT'55';
 /* '55' S3(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
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 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,23;
 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'56' DELTA-STRGTH-FUNCT'56'
 (MEV) (UNIT) (UNIT)
 8.512E+00 5547 +5547-5547
 9.488E+00 5309 +5388-5388
 1.150E+01 52850 +25360-25360
 1.251E+01 74880 +21080-20520
 1.351E+01 53570 +24330-25200
 1.450E+01 42000 +15210-15930
 1.551E+01 61250 +15770-14980
 1.650E+01 55710 +14660-14660
 1.749E+01 69180 +18620-14100
 1.850E+01 53490 +12200-12200
 1.951E+01 47620 +14500-18860
 2.052E+01 54440 +17590-17590
 2.151E+01 58870 +18460-14980
 2.250E+01 42160 +13070-13070
 2.350E+01 44370 +15370-15370
 2.451E+01 32170 +13070-13070
 2.550E+01 29080 +13230-15450
 2.650E+01 27100 +15450-15450
 2.751E+01 16400 +16480-16480
 2.850E+01 12440 +12440-12440
 3.051E+01 8399 +8558-8558
 3.149E+01 11650 +11570-11570
 \END;
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