/*===================================================================*/
 /* NRDF D1899 Data No.11                                             */
 /*===================================================================*/
 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,11;
 D#=D1899;
 TITLE=/ Systematics of the bimodal isoscalar giant dipole resonance
 ATH=(M.UCHIDA'1', H.SAKAGUCHI'1', M.ITOH'1', M.YOSOI'1', T.KAWABATA'1',
      Y.YASUDA'1', H.TAKEDA'1', T.MURAKAMI'1', S.TERASHIMA'1',
      S.KISHI'1', U.GARG'2', P.BOUTACHKOV'2', M.HEDDEN'2',
      B.KHARRAJA'2', M.KOSS'2', B.K.NAYAK'2', S.ZHU'2', M.FUJIWARA'3,4',
      H.FUJIMURA'3', H.P.YOSHIDA'3', K.HARA'3', H.AKIMUNE'5',
      M.N.HARAKEH'6');
 INST-ATH=(2JPNKTO'1', 1USANOT'2', 2JPNRCN'3', 2JPNJAE'4', 2JPNKON'5',
           2NEDKVI'6');
      /* '1' Department of Physics */
      /* '2' Physics Department */
      /* '4' Advanced Science Research Center */
      /* '5' Department of Physics */
 REF=PR/C;
 VLP=69(2004)051301;
 /* Secondary references 
    - Uchida, Thesis(2003)
    - 2007TOKYO, 2(2007)314 (T.Li et al., DA/DE and DA for 112SN and
      124Sn given)
 RCTS=(90ZR(ALPHA,INL), 116SN(ALPHA,INL), 208PB(ALPHA,INL),
       208PB(ALPHA,ALPHA)208PB, 144SM(ALPHA,ALPHA)144SM,
       116SN(ALPHA,ALPHA)116SN, 90ZR(ALPHA,ALPHA)90ZR,
       58NI(ALPHA,ALPHA)58NI, 12C(ALPHA,ALPHA)12C, 58NI(ALPHA,INL));
 PHQS=(ENGY-SPEC, ANGL-DSTRN, STRGTH-FUNCT'7', STRGTH-FUNCT'8', EWSR,
       DBL-DIFF-XSECTN);
 /* '7' Strength distribution for T=0, L=0 transitions, ISGMR */
 /* '8' Strength distribution for T=0, L=1 transitions, ISGDR */
 /*===================================================================*/
 /* Experimental Conditions                                           */
 /*===================================================================*/
 \\EXP,11;
 /* 2004-11-07 : Compiled+Checked, Kc + Sr + On */
 /* 2010-01-08 : Altered, Nf. REFERENCE: 2007TOKYO added */
 /* Related references 
    - M.Itoh et al., PR/C, 68(2003)064602.
    (Spectrum for 144Sm shown in Fig.1(c) of the main reference given).
    See also NRDF D1886 DATA 1.
 ENR=X%;
 CHM=ELM;
 PHYS-FORM=SLD;
 BAC=SELF;
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=CYC'9';
 /* '9' Ring cyclotron */
 INST-ACC=2JPNRCN;
 INC-ENGY-LAB-RANGE=386MEV;
 CHRG-INC-ION=+2;
 POL-PRJ=0%;
 DET-PARTCL=ALPHA;
 COINC=NO;
 ANT-COINC=NO;
 DET-SYS=(MAG'10',MWDC'11',SCT'12');
 /* '10' To analyze inelastically scattered particles, Grand
         Raiden [M.Fujiwara et al., Nucl. Instrum. Methods Phys. Res. A
         422, 484 (1999)]. */
 /* '11' Focal-plane detection system [T. Noro et al., RCNP Annual
         Report, 1991, p177] */
 /* '12' Two plastic scintillation counters. Focal-plane detection
         system. */
 RCT=208PB(ALPHA,INL);
 RTY=INEL-SCATT;
 PHQ=STRGTH-FUNCT'23';
 /* '23' Strength distribution for T=0, L=1 transitions, ISGDR */
 /* Analysis:
    - DWBA cross sections with multipole decomposition analysis
      [B.Bonin et al., Nucl. Phys. A 430, 349(1984). ] are used to
      obtain strength distributions.
    - Fitting with Breit-Wigner functions and Gaussian function for
      each energy regions.
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,11;
 INC-ENGY-LAB=386MEV;
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 EXC-ENGY STRGTH-FUNCT'24' DELTA-STRGTH-FUNCT'24'
 (MEV) (FM**6/MEV) (FM**6/MEV)
 8.521E+00 1.901E+03 +-2.161E+02
 9.553E+00 9.123E+02 +-3.061E+02
 1.053E+01 8.598E+02 +-3.601E+02
 1.150E+01 2.644E+03 +-6.304E+02
 1.251E+01 4.410E+03 +-7.022E+02
 1.349E+01 4.682E+03 +-7.204E+02
 1.448E+01 3.207E+03 +-5.402E+02
 1.556E+01 2.110E+03 +-3.601E+02
 1.649E+01 2.634E+03 +-3.240E+02
 1.751E+01 2.978E+03 +-2.881E+02
 1.849E+01 3.754E+03 +-3.782E+02
 1.946E+01 4.368E+03 +-3.421E+02
 2.044E+01 4.819E+03 +-3.422E+02
 2.150E+01 5.235E+03 +-3.602E+02
 2.253E+01 5.507E+03 +-4.682E+02
 2.355E+01 4.950E+03 +-3.780E+02
 2.458E+01 4.736E+03 +-3.960E+02
 2.552E+01 4.431E+03 +-3.421E+02
 2.646E+01 4.000E+03 +-3.961E+02
 2.748E+01 3.642E+03 +-5.943E+02
 2.846E+01 4.256E+03 +-4.683E+02
 2.948E+01 4.329E+03 +-3.781E+02
 3.047E+01 3.592E+03 +-4.682E+02
 3.153E+01 4.422E+03 +-5.402E+02
 \END;
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