DARPE: Search Results
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 /* NRDF D1796 Data No.7                                              */
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 /* Bibliography                                                      */
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 \\BIB,7;
 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. */
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 /* Experimental Conditions                                           */
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 \\EXP,7;
 /* 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=144SM(ALPHA,ALPHA)144SM;
 PHQ=ANGL-DSTRN'21';
 /* '21' Double differential cross section with scattered alpha
         particle. */
 ANL=DWBA'22';
 /* '22' Multipole-decomposition (MD) analysis [B. Bonin et al.,
         Nucl. Phys. A 430 (1984) 349] with DWBA code ECIS95 [J.
         Raynal, Computer Code, ECIS95, NEA0850-14]. */
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 /* Descriptive Parameters                                            */
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 \\DATA,7;
 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)). */
 EXC-ENGY=15.5MEV;
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 /* Data Table                                                        */
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 \DATA;
 THTC DSIGMA/DOMEGA/DE DELTA-DSIGMA/DOMEGA/DE
 (DEG) (MB/SR/MEV) (MB/SR/MEV)
 0.694 1.4863e+02 +-1.0328e+00
 1.487 7.8145e+01 +-1.3189e+00
 2.028 5.4494e+01 +-7.6193e-01
 2.413 5.2874e+01 +-7.0154e-01
 2.804 5.5757e+01 +-7.0989e-01
 3.000 5.4494e+01 +-6.6975e-01
 3.197 5.5317e+01 +-7.3436e-01
 3.395 5.1598e+01 +-6.4914e-01
 3.791 4.2762e+01 +-6.2035e-01
 4.189 3.3828e+01 +-5.1909e-01
 4.488 2.9856e+01 +-3.7213e-01
 4.887 2.9695e+01 +-3.7316e-01
 5.287 2.9200e+01 +-3.7348e-01
 5.688 2.7603e+01 +-4.5144e-01
 5.988 2.1003e+01 +-2.8560e-01
 6.389 1.7177e+01 +-2.3427e-01
 6.791 1.3558e+01 +-2.0684e-01
 7.192 1.1877e+01 +-1.9340e-01
 7.493 1.1374e+01 +-1.8581e-01
 7.895 1.1158e+01 +-1.8559e-01
 8.297 1.0778e+01 +-1.8134e-01
 8.699 9.1092e+00 +-1.6670e-01
 9.000 7.4278e+00 +-1.5136e-01
 9.402 5.9449e+00 +-1.3535e-01
 9.804 5.4756e+00 +-1.3155e-01
 10.207 5.2899e+00 +-1.2799e-01
 10.508 4.5971e+00 +-1.1263e-01
 10.910 4.2362e+00 +-1.0809e-01
 11.313 3.7829e+00 +-1.0309e-01
 11.715 3.1475e+00 +-9.2981e-02
 12.017 2.5872e+00 +-7.3761e-02
 12.419 2.4755e+00 +-7.2529e-02
 12.821 2.3481e+00 +-7.0787e-02
 13.223 1.9242e+00 +-6.3684e-02
 \END;
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