DARPE: Search Results
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 /* NRDF D1796 Data No.12                                             */
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 /* Bibliography                                                      */
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 \\BIB,12;
 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,12;
 /* 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=154SM(ALPHA,ALPHA)154SM;
 PHQ=ANGL-DSTRN'31';
 /* '31' Double differential cross section with scattered alpha
         particle. */
 ANL=DWBA'32';
 /* '32' 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,12;
 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=22.5MEV;
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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)
 0.686 4.9634e+01 +-1.0633e+00
 1.469 4.3622e+01 +-2.0289e+00
 2.004 3.8308e+01 +-8.3696e-01
 2.385 3.6865e+01 +-6.9803e-01
 2.770 3.5573e+01 +-6.6937e-01
 2.965 3.6248e+01 +-5.6612e-01
 3.159 3.2635e+01 +-6.1549e-01
 3.355 3.5888e+01 +-5.7327e-01
 3.747 3.4401e+01 +-5.8087e-01
 4.140 3.1848e+01 +-5.3556e-01
 4.435 3.1113e+01 +-4.5767e-01
 4.830 2.8146e+01 +-4.3975e-01
 5.225 2.4730e+01 +-4.1559e-01
 5.621 2.1682e+01 +-3.9017e-01
 5.918 1.8567e+01 +-2.8951e-01
 6.314 1.6223e+01 +-5.6682e-01
 6.710 1.4591e+01 +-6.3006e-01
 7.107 1.1228e+01 +-4.2318e-01
 7.405 8.5731e+00 +-1.5578e-01
 7.802 7.4415e+00 +-1.4498e-01
 8.199 7.0134e+00 +-1.4144e-01
 8.596 6.3802e+00 +-1.3365e-01
 \END;
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