DARPE: Search Results
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 /* NRDF D1796 Data No.9                                              */
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 /* Bibliography                                                      */
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 \\BIB,9;
 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,9;
 /* 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'25';
 /* '25' Double differential cross section with scattered alpha
         particle. */
 ANL=DWBA'26';
 /* '26' 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,9;
 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=25.5MEV;
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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)
 0.684 4.2281e+01 +-5.3825e-01
 1.466 3.9748e+01 +-1.0841e+00
 1.999 3.1831e+01 +-7.2497e-01
 2.379 2.9657e+01 +-5.8219e-01
 2.764 2.7468e+01 +-4.9704e-01
 2.958 2.6409e+01 +-4.2884e-01
 3.152 2.6501e+01 +-5.5335e-01
 3.347 2.6328e+01 +-4.1277e-01
 3.738 2.5646e+01 +-4.2762e-01
 4.130 2.4422e+01 +-4.3578e-01
 4.425 2.2387e+01 +-2.9923e-01
 4.818 2.0014e+01 +-2.8493e-01
 5.212 1.8127e+01 +-2.7134e-01
 5.607 1.5672e+01 +-2.5527e-01
 5.903 1.4719e+01 +-2.1174e-01
 6.299 1.3462e+01 +-2.0387e-01
 6.694 1.1989e+01 +-1.9355e-01
 7.090 1.0567e+01 +-2.2599e-01
 7.387 9.4531e+00 +-2.2735e-01
 7.783 8.0491e+00 +-1.6199e-01
 8.179 7.2364e+00 +-1.5046e-01
 8.575 6.4771e+00 +-1.4147e-01
 8.872 6.2719e+00 +-1.3941e-01
 9.268 5.5055e+00 +-1.3181e-01
 9.665 4.7561e+00 +-1.2295e-01
 10.061 4.0152e+00 +-1.1213e-01
 10.358 3.4030e+00 +-9.7335e-02
 10.754 3.2675e+00 +-9.4019e-02
 11.151 2.9886e+00 +-9.1085e-02
 11.547 2.5586e+00 +-8.4285e-02
 11.844 2.3400e+00 +-6.9927e-02
 12.241 2.1244e+00 +-6.7355e-02
 12.637 1.7931e+00 +-6.2223e-02
 13.033 1.6520e+00 +-5.9703e-02
 \END;
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