/*===================================================================*/ /* NRDF D1899 Data No.6 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,6; D#=D1899; TITLE=/ Systematics of the bimodal isoscalar giant dipole resonance ATH=(M.UCHIDA'1', H.SAKAGUCHI'1', M.ITOH'1', M.YOSOI'1', T.KAWABATA'1', Y.YASUDA'1', H.TAKEDA'1', T.MURAKAMI'1', S.TERASHIMA'1', S.KISHI'1', U.GARG'2', P.BOUTACHKOV'2', M.HEDDEN'2', B.KHARRAJA'2', M.KOSS'2', B.K.NAYAK'2', S.ZHU'2', M.FUJIWARA'3,4', H.FUJIMURA'3', H.P.YOSHIDA'3', K.HARA'3', H.AKIMUNE'5', M.N.HARAKEH'6'); INST-ATH=(2JPNKTO'1', 1USANOT'2', 2JPNRCN'3', 2JPNJAE'4', 2JPNKON'5', 2NEDKVI'6'); /* '1' Department of Physics */ /* '2' Physics Department */ /* '4' Advanced Science Research Center */ /* '5' Department of Physics */ REF=PR/C; VLP=69(2004)051301; /* Secondary references - Uchida, Thesis(2003) - 2007TOKYO, 2(2007)314 (T.Li et al., DA/DE and DA for 112SN and 124Sn given) RCTS=(90ZR(ALPHA,INL), 116SN(ALPHA,INL), 208PB(ALPHA,INL), 208PB(ALPHA,ALPHA)208PB, 144SM(ALPHA,ALPHA)144SM, 116SN(ALPHA,ALPHA)116SN, 90ZR(ALPHA,ALPHA)90ZR, 58NI(ALPHA,ALPHA)58NI, 12C(ALPHA,ALPHA)12C, 58NI(ALPHA,INL)); PHQS=(ENGY-SPEC, ANGL-DSTRN, STRGTH-FUNCT'7', STRGTH-FUNCT'8', EWSR, DBL-DIFF-XSECTN); /* '7' Strength distribution for T=0, L=0 transitions, ISGMR */ /* '8' Strength distribution for T=0, L=1 transitions, ISGDR */ /*===================================================================*/ /* Experimental Conditions */ /*===================================================================*/ \\EXP,6; /* 2004-11-07 : Compiled+Checked, Kc + Sr + On */ /* 2010-01-08 : Altered, Nf. REFERENCE: 2007TOKYO added */ /* Related references - M.Itoh et al., PR/C, 68(2003)064602. (Spectrum for 144Sm shown in Fig.1(c) of the main reference given). See also NRDF D1886 DATA 1. ENR=X%; CHM=ELM; PHYS-FORM=SLD; BAC=SELF; POL-TGT=0%; ALGN-TGT=0%; ACC=CYC'9'; /* '9' Ring cyclotron */ INST-ACC=2JPNRCN; INC-ENGY-LAB-RANGE=386MEV; CHRG-INC-ION=+2; POL-PRJ=0%; DET-PARTCL=ALPHA; COINC=NO; ANT-COINC=NO; DET-SYS=(MAG'10',MWDC'11',SCT'12'); /* '10' To analyze inelastically scattered particles, Grand Raiden [M.Fujiwara et al., Nucl. Instrum. Methods Phys. Res. A 422, 484 (1999)]. */ /* '11' Focal-plane detection system [T. Noro et al., RCNP Annual Report, 1991, p177] */ /* '12' Two plastic scintillation counters. Focal-plane detection system. */ RCT=90ZR(ALPHA,INL); RTY=INEL-SCATT; PHQ=STRGTH-FUNCT'13'; /* '13' Strength distribution for T=0, L=0 transitions, ISGMR */ /* Analysis: - DWBA cross sections with multipole decomposition analysis [B.Bonin et al., Nucl. Phys. A 430, 349(1984). ] are used to obtain strength distributions. /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,6; INC-ENGY-LAB=386MEV; /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; EXC-ENGY STRGTH-FUNCT'14' DELTA-STRGTH-FUNCT'14' (MEV) (FM**4/MEV) (FM**4/MEV) 8.491E+00 8.734E+01 +-1.924E+01 9.503E+00 1.422E+02 +-1.924E+01 1.052E+01 9.113E+01 +-2.567E+01 1.146E+01 1.588E+02 +-2.888E+01 1.257E+01 2.265E+02 +-3.529E+01 1.348E+01 4.738E+02 +-1.603E+01 1.453E+01 6.281E+02 +-5.453E+01 1.547E+01 9.845E+02 +-6.417E+01 1.652E+01 1.216E+03 +-6.738E+01 1.756E+01 9.915E+02 +-5.454E+01 1.850E+01 7.159E+02 +-5.453E+01 1.955E+01 5.333E+02 +-3.529E+01 2.056E+01 4.405E+02 +-4.171E+01 2.154E+01 3.959E+02 +-4.813E+01 2.259E+01 3.737E+02 +-4.491E+01 2.349E+01 3.740E+02 +-3.529E+01 2.461E+01 3.743E+02 +-4.492E+01 2.559E+01 3.586E+02 +-5.453E+01 2.656E+01 2.882E+02 +-6.737E+01 2.758E+01 3.078E+02 +-4.812E+01 2.859E+01 2.696E+02 +-6.416E+01 2.959E+01 2.522E+02 +-6.472E+01 3.054E+01 2.913E+02 +-5.827E+01 3.164E+01 2.657E+02 +-7.118E+01 \END; /*===================================================================*/ |