DARPE: Search Results
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 /* NRDF D1796 Data No.20                                             */
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 /* Bibliography                                                      */
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 \\BIB,20;
 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,20;
 /* 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. */
 /* 2006-09-08 : Altered, Mt. Re-digitized */
 RCT=144SM(ALPHA,ALPHA)144SM;
 PHQ=STRGTH-FUNCT'49';
 /* '49' S1(Ex) : The definition is shown in reference. */
 /* Analysis:
    - multipole-decomposition (MD) analysis. [B. Bonin et al., Nucl.
      Phys. A 430 (1984) 349]
    - Breit-Wigner fits
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 /* Descriptive Parameters                                            */
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 \\DATA,20;
 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)). */
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 /* Data Table                                                        */
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 \DATA;
 EXC-ENGY STRGTH-FUNCT'50' DELTA-STRGTH-FUNCT'50'
 (MEV) (UNIT) (UNIT)
 8.510E+00 261.4 +NEGLIGIBLE-NEGLIGIBLE
 9.501E+00 269.8 +30.4-21.28
 1.050E+01 299.4 +42.55-42.55
 1.151E+01 370.1 +44.07-44.07
 1.251E+01 426.3 +53.19-53.19
 1.350E+01 466.6 +46.35-46.35
 1.451E+01 513.7 +37.23-37.23
 1.551E+01 496.2 +40.27-40.27
 1.650E+01 414.1 +30.4-30.4
 1.750E+01 377.7 +23.56-23.56
 1.850E+01 372.3 +28.12-28.12
 1.949E+01 390.6 +31.16-31.16
 2.051E+01 395.9 +25.08-25.08
 2.151E+01 486.3 +29.64-29.64
 2.250E+01 509.9 +34.19-34.19
 2.350E+01 518.2 +37.23-37.23
 2.450E+01 566.1 +28.12-28.12
 2.550E+01 555.5 +33.43-33.43
 2.650E+01 506.1 +26.6-26.6
 2.750E+01 471.9 +36.47-36.47
 2.850E+01 493.2 +34.95-34.95
 2.949E+01 458.2 +31.91-31.91
 3.049E+01 466.6 +51.67-51.67
 3.149E+01 443.8 +40.27-40.27
 3.249E+01 429.3 +50.15-50.15
 \END;
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