/*===================================================================*/ /* NRDF D1796 Data No.19 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,19; 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. */ /*===================================================================*/ /* Experimental Conditions */ /*===================================================================*/ \\EXP,19; /* 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=154SM(ALPHA,ALPHA)154SM; PHQ=STRGTH-FUNCT'47'; /* '47' S2(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 /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,19; 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)). */ /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; EXC-ENGY STRGTH-FUNCT'48' DELTA-STRGTH-FUNCT'48' (MEV) (UNIT) (UNIT) 8.948E+00 1631 +-822.9 9.887E+00 1883 +-278 1.083E+01 2569 +-215 1.174E+01 3540 +-218.7 1.268E+01 3981 +-307.6 1.357E+01 3529 +-270.6 1.448E+01 3095 +-329.9 1.542E+01 2602 +-203.9 1.633E+01 2128 +-196.4 1.729E+01 1939 +-215 1.820E+01 1801 +-185.3 1.911E+01 1694 +-163.1 2.004E+01 1468 +-211.3 2.094E+01 1483 +-233.5 2.188E+01 1408 +-185.3 2.279E+01 1345 +-174.2 2.373E+01 1312 +-229.8 2.465E+01 1201 +-185.3 2.556E+01 1223 +-189 2.652E+01 1197 +-215 2.741E+01 1216 +-244.6 2.835E+01 1138 +-189 2.926E+01 1282 +-200.2 3.020E+01 1004 +-289.1 3.111E+01 1197 +-248.3 3.202E+01 1131 +-259.5 \END; /*===================================================================*/ |