/*===================================================================*/ /* NRDF D1796 Data No.5 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,5; 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,5; /* 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=ENGY-SPEC; /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,5; 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)). */ THTL=[0.7DEG; /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; EXC-ENGY DSIGMA/DOMEGA/DE DELTA-DSIGMA/DOMEGA/DE (MEV) (MB/SR/MEV) (MB/SR/MEV) 8.125 0.64987E+02 +-0.80615E+01 8.375 0.62211E+02 +-0.78874E+01 8.625 0.72779E+02 +-0.85311E+01 8.875 0.72180E+02 +-0.84959E+01 9.125 0.82149E+02 +-0.90636E+01 9.375 0.87133E+02 +-0.93345E+01 9.625 0.91550E+02 +-0.95682E+01 9.875 0.95967E+02 +-0.97963E+01 10.125 0.10269E+03 +-0.10133E+02 10.375 0.10934E+03 +-0.10457E+02 10.625 0.11149E+03 +-0.10559E+02 10.875 0.12436E+03 +-0.11152E+02 11.125 0.12830E+03 +-0.11327E+02 11.375 0.13351E+03 +-0.11555E+02 11.625 0.13770E+03 +-0.11735E+02 11.875 0.14174E+03 +-0.11906E+02 12.125 0.14427E+03 +-0.12011E+02 12.375 0.13363E+03 +-0.11560E+02 12.625 0.13695E+03 +-0.11702E+02 12.875 0.13493E+03 +-0.11616E+02 13.125 0.13414E+03 +-0.11582E+02 13.375 0.13423E+03 +-0.11586E+02 13.625 0.13004E+03 +-0.11403E+02 13.875 0.13903E+03 +-0.11791E+02 14.125 0.13370E+03 +-0.11563E+02 14.375 0.13827E+03 +-0.11759E+02 14.625 0.12950E+03 +-0.11380E+02 14.875 0.14117E+03 +-0.11882E+02 15.125 0.13764E+03 +-0.11732E+02 15.375 0.13190E+03 +-0.11485E+02 15.625 0.13247E+03 +-0.11509E+02 15.875 0.12890E+03 +-0.11353E+02 16.125 0.11978E+03 +-0.10945E+02 16.375 0.11370E+03 +-0.10663E+02 16.625 0.10619E+03 +-0.10305E+02 16.875 0.95935E+02 +-0.97946E+01 17.125 0.87638E+02 +-0.93615E+01 17.375 0.78174E+02 +-0.88416E+01 17.625 0.80130E+02 +-0.89515E+01 17.875 0.71170E+02 +-0.84363E+01 18.125 0.73379E+02 +-0.85661E+01 18.375 0.63820E+02 +-0.79887E+01 18.625 0.67069E+02 +-0.81896E+01 18.875 0.60287E+02 +-0.77645E+01 19.125 0.60823E+02 +-0.77989E+01 19.375 0.59309E+02 +-0.77012E+01 19.625 0.51801E+02 +-0.71973E+01 19.875 0.60791E+02 +-0.77969E+01 20.125 0.58015E+02 +-0.76168E+01 20.375 0.57069E+02 +-0.75544E+01 20.625 0.60224E+02 +-0.77604E+01 20.875 0.56533E+02 +-0.75188E+01 21.125 0.53883E+02 +-0.73405E+01 21.375 0.51990E+02 +-0.72104E+01 21.625 0.54009E+02 +-0.73491E+01 21.875 0.53441E+02 +-0.73103E+01 22.125 0.55681E+02 +-0.74620E+01 22.375 0.53536E+02 +-0.73168E+01 22.625 0.47731E+02 +-0.69088E+01 22.875 0.53441E+02 +-0.73103E+01 23.125 0.51958E+02 +-0.72082E+01 23.375 0.51233E+02 +-0.71577E+01 23.625 0.47699E+02 +-0.69065E+01 23.875 0.48867E+02 +-0.69905E+01 24.125 0.50633E+02 +-0.71157E+01 24.375 0.46879E+02 +-0.68468E+01 24.625 0.44040E+02 +-0.66363E+01 24.875 0.46343E+02 +-0.68076E+01 25.125 0.44040E+02 +-0.66363E+01 25.375 0.40538E+02 +-0.63670E+01 25.625 0.41737E+02 +-0.64604E+01 25.875 0.42589E+02 +-0.65260E+01 26.125 0.42589E+02 +-0.65260E+01 26.375 0.41074E+02 +-0.64089E+01 26.625 0.40822E+02 +-0.63892E+01 26.875 0.37888E+02 +-0.61553E+01 27.125 0.39245E+02 +-0.62646E+01 27.375 0.37005E+02 +-0.60832E+01 27.625 0.35901E+02 +-0.59917E+01 27.875 0.36405E+02 +-0.60337E+01 28.125 0.38866E+02 +-0.62343E+01 28.375 0.37794E+02 +-0.61476E+01 28.625 0.32084E+02 +-0.56642E+01 28.875 0.34765E+02 +-0.58962E+01 29.125 0.35522E+02 +-0.59600E+01 29.375 0.36311E+02 +-0.60258E+01 29.625 0.35017E+02 +-0.59175E+01 29.875 0.32399E+02 +-0.56920E+01 30.125 0.37951E+02 +-0.61605E+01 30.375 0.37667E+02 +-0.61374E+01 30.625 0.32778E+02 +-0.57252E+01 30.875 0.30695E+02 +-0.55403E+01 31.125 0.36847E+02 +-0.60702E+01 31.375 0.31768E+02 +-0.56363E+01 31.625 0.32052E+02 +-0.56614E+01 31.875 0.30317E+02 +-0.55061E+01 32.125 0.31011E+02 +-0.55687E+01 32.375 0.27572E+02 +-0.52509E+01 32.625 0.31610E+02 +-0.56223E+01 32.875 0.30569E+02 +-0.55289E+01 33.125 0.31358E+02 +-0.55998E+01 33.375 0.27667E+02 +-0.52599E+01 33.625 0.30727E+02 +-0.55432E+01 33.875 0.32399E+02 +-0.56920E+01 34.125 0.28519E+02 +-0.53403E+01 34.375 0.30506E+02 +-0.55232E+01 34.625 0.30412E+02 +-0.55147E+01 34.875 0.28771E+02 +-0.53639E+01 \END; /*===================================================================*/ |