DARPE: Search Results
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 /* NRDF D1796 Data No.11                                             */
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 /* Bibliography                                                      */
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 \\BIB,11;
 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,11;
 /* 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'29';
 /* '29' Double differential cross section with scattered alpha
         particle. */
 ANL=DWBA'30';
 /* '30' 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,11;
 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)
 0.693 1.2531e+02 +-1.2576e+00
 1.484 8.2216e+01 +-2.3523e+00
 2.024 5.7002e+01 +-8.7616e-01
 2.408 5.5987e+01 +-8.1383e-01
 2.798 5.8151e+01 +-8.0010e-01
 2.994 5.6302e+01 +-7.1961e-01
 3.191 5.3219e+01 +-7.6830e-01
 3.388 5.3280e+01 +-6.8948e-01
 3.784 4.5009e+01 +-6.7315e-01
 4.181 3.7694e+01 +-5.9452e-01
 4.479 3.4584e+01 +-4.8151e-01
 4.878 3.2695e+01 +-4.7978e-01
 5.277 3.3210e+01 +-1.1233e+00
 5.677 3.0963e+01 +-1.2601e+00
 5.977 2.2610e+01 +-7.9886e-01
 6.377 1.9247e+01 +-2.9466e-01
 6.778 1.4800e+01 +-2.5737e-01
 7.178 1.2605e+01 +-2.3662e-01
 7.479 1.0019e+01 +-1.6784e-01
 7.880 9.9727e+00 +-1.6801e-01
 8.281 9.0276e+00 +-1.5991e-01
 8.682 7.4563e+00 +-1.4428e-01
 \END;
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