DARPE: Search Results
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 /* NRDF D1796 Data No.15                                             */
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 /* Bibliography                                                      */
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 \\BIB,15;
 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,15;
 /* 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. */
 RCT=204PB(P,T)202PB;
 CHM=ELM'74';
 /* '74' Prepared by centrifugal settling of PbO */
 PHYS-FORM=SLD;
 THK-TGT=2MG/CM**2;
 BAC=MYLAR;
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 /* Descriptive Parameters                                            */
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 \\DATA,15;
 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)). */
 INC-ENGY-LAB=51.9MEV;
 SYS-ERR=<20%'75';
 /* '75' Error of the absolute cross section of the ground state
         transition is estimated to be less than 20%, where the main
         part comes from the uncertainty of the solid angle of each
         counter on the focal plane of the magnetic spectrograph. */
 EMT=T;
 RSD=202PB;
 EXC-ENGY=0.95MEV;
 J-PTY=2+;
 DELTA-THTC=0.25DEG'76';
 /* '76' Data-point reader uncertainty */
 DELTA-DSIGMA/DOMEGA=1.9%'77';
 /* '77' Data-point reader uncertainty */
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 /* Data Table                                                        */
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 \DATA;
 THTC DSIGMA/DOMEGA
 (DEG) (UB/SR)
 4.38           118.2
 6.01           126.6
 8.18           117.
 10.53          106.7
 13.24          85.
 15.41          77.5
 17.94          73.6
 20.1           58.6
 23.            36.1
 25.35          25.8
 28.06          19.
 30.95          21.5
 33.11          23.3
 35.47          21.9
 38.            14.8
 43.06          10.18
 47.94          10.23
 \END;
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