/*===================================================================*/
 /* NRDF D1899 Data No.8                                              */
 /*===================================================================*/
 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,8;
 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,8;
 /* 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=116SN(ALPHA,INL);
 RTY=INEL-SCATT;
 PHQ=STRGTH-FUNCT'17';
 /* '17' Strength distribution for T=0, L=0 transitions, ISGMR */
 /* 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 a Breit-Wigner function
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,8;
 INC-ENGY-LAB=386MEV;
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 EXC-ENGY STRGTH-FUNCT'18' DELTA-STRGTH-FUNCT'18'
 (MEV) (FM**4/MEV) (FM**4/MEV)
 8.556E+00 4.014E+02 +-3.369E+01
 9.553E+00 3.003E+02 +-5.295E+01
 1.059E+01 3.581E+02 +-4.332E+01
 1.149E+01 5.795E+02 +-3.369E+01
 1.256E+01 8.153E+02 +-6.257E+01
 1.355E+01 1.080E+03 +-1.011E+02
 1.449E+01 1.460E+03 +-9.145E+01
 1.552E+01 1.648E+03 +-1.348E+02
 1.648E+01 1.441E+03 +-1.059E+02
 1.757E+01 9.982E+02 +-9.145E+01
 1.849E+01 7.239E+02 +-7.220E+01
 1.961E+01 5.410E+02 +-5.776E+01
 2.048E+01 5.265E+02 +-8.183E+01
 2.152E+01 5.362E+02 +-7.701E+01
 2.251E+01 5.025E+02 +-8.664E+01
 2.346E+01 4.928E+02 +-9.145E+01
 2.458E+01 4.447E+02 +-8.664E+01
 2.553E+01 4.591E+02 +-7.701E+01
 2.653E+01 4.688E+02 +-1.011E+02
 2.752E+01 4.447E+02 +-1.011E+02
 2.852E+01 3.966E+02 +-9.627E+01
 2.951E+01 3.918E+02 +-1.059E+02
 3.054E+01 4.254E+02 +-1.107E+02
 3.154E+01 4.880E+02 +-1.107E+02
 \END;
 /*===================================================================*/