DARPE: Search Results
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 /* NRDF D1796 Data No.6                                              */
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 /* Bibliography                                                      */
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 \\BIB,6;
 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,6;
 /* 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'19';
 /* '19' Double differential cross section with scattered alpha
         particle. */
 ANL=DWBA'20';
 /* '20' 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,6;
 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=11.5MEV;
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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)
 0.698 7.5753e+01 +-9.0475e-01
 1.495 6.2203e+01 +-1.1476e+00
 2.039 5.6339e+01 +-7.4363e-01
 2.427 6.1829e+01 +-7.2005e-01
 2.819 6.6489e+01 +-7.3021e-01
 3.017 6.7172e+01 +-7.4655e-01
 3.215 6.4692e+01 +-7.7610e-01
 3.414 5.6539e+01 +-7.0920e-01
 3.813 4.3876e+01 +-6.0775e-01
 4.213 3.3890e+01 +-5.0993e-01
 4.513 3.0227e+01 +-3.8072e-01
 4.915 3.2252e+01 +-5.1867e-01
 5.317 3.1247e+01 +-3.9919e-01
 5.720 2.8919e+01 +-3.6558e-01
 6.022 2.1983e+01 +-2.6403e-01
 6.425 1.6719e+01 +-2.3196e-01
 6.829 1.2739e+01 +-2.0174e-01
 7.233 1.2078e+01 +-1.9310e-01
 7.535 1.2216e+01 +-1.9290e-01
 7.939 1.2369e+01 +-1.9426e-01
 8.344 1.0976e+01 +-1.8406e-01
 8.748 9.0414e+00 +-1.6697e-01
 9.051 7.3526e+00 +-1.5067e-01
 9.455 5.7118e+00 +-1.3466e-01
 9.860 5.1793e+00 +-1.2734e-01
 10.264 4.9562e+00 +-1.2468e-01
 10.568 5.2752e+00 +-1.2039e-01
 10.972 4.7757e+00 +-1.1473e-01
 11.377 4.0532e+00 +-1.0499e-01
 11.781 3.1561e+00 +-9.3115e-02
 12.085 2.5251e+00 +-7.3311e-02
 12.490 2.2288e+00 +-6.8504e-02
 12.894 2.1917e+00 +-6.8763e-02
 13.299 2.0603e+00 +-6.6110e-02
 \END;
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