/*===================================================================*/ /* NRDF D1796 Data No.3 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,3; 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,3; /* 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=150SM(ALPHA,ALPHA)150SM; PHQ=ENGY-SPEC; /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,3; 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 0.65868E+02 +-0.81159E+01 8.375 0.67070E+02 +-0.81896E+01 8.625 0.64889E+02 +-0.80554E+01 8.875 0.68384E+02 +-0.82695E+01 9.125 0.69484E+02 +-0.83357E+01 9.375 0.74294E+02 +-0.86194E+01 9.625 0.78614E+02 +-0.88664E+01 9.875 0.82814E+02 +-0.91002E+01 10.125 0.87812E+02 +-0.93708E+01 10.375 0.92287E+02 +-0.96066E+01 10.625 0.95001E+02 +-0.97469E+01 10.875 0.10356E+03 +-0.10177E+02 11.125 0.10865E+03 +-0.10423E+02 11.375 0.11729E+03 +-0.10830E+02 11.625 0.11952E+03 +-0.10933E+02 11.875 0.12749E+03 +-0.11291E+02 12.125 0.13585E+03 +-0.11655E+02 12.375 0.13065E+03 +-0.11430E+02 12.625 0.13445E+03 +-0.11595E+02 12.875 0.13801E+03 +-0.11748E+02 13.125 0.14222E+03 +-0.11926E+02 13.375 0.14157E+03 +-0.11898E+02 13.625 0.14801E+03 +-0.12166E+02 13.875 0.15485E+03 +-0.12444E+02 14.125 0.14690E+03 +-0.12120E+02 14.375 0.14540E+03 +-0.12058E+02 14.625 0.14595E+03 +-0.12081E+02 14.875 0.15175E+03 +-0.12319E+02 15.125 0.14756E+03 +-0.12147E+02 15.375 0.14164E+03 +-0.11901E+02 15.625 0.13059E+03 +-0.11428E+02 15.875 0.12400E+03 +-0.11135E+02 16.125 0.11816E+03 +-0.10870E+02 16.375 0.11028E+03 +-0.10501E+02 16.625 0.10043E+03 +-0.10021E+02 16.875 0.92227E+02 +-0.96035E+01 17.125 0.84222E+02 +-0.91773E+01 17.375 0.79112E+02 +-0.88945E+01 17.625 0.78107E+02 +-0.88378E+01 17.875 0.68256E+02 +-0.82617E+01 18.125 0.73598E+02 +-0.85789E+01 18.375 0.75032E+02 +-0.86621E+01 18.625 0.69355E+02 +-0.83280E+01 18.875 0.63884E+02 +-0.79927E+01 19.125 0.60440E+02 +-0.77743E+01 19.375 0.62819E+02 +-0.79258E+01 19.625 0.63119E+02 +-0.79448E+01 19.875 0.64021E+02 +-0.80013E+01 20.125 0.60319E+02 +-0.77666E+01 20.375 0.58997E+02 +-0.76809E+01 20.625 0.57691E+02 +-0.75955E+01 20.875 0.59546E+02 +-0.77166E+01 21.125 0.60371E+02 +-0.77699E+01 21.375 0.62132E+02 +-0.78824E+01 21.625 0.60268E+02 +-0.77632E+01 21.875 0.58748E+02 +-0.76647E+01 22.125 0.60500E+02 +-0.77782E+01 22.375 0.59212E+02 +-0.76949E+01 22.625 0.59598E+02 +-0.77200E+01 22.875 0.62501E+02 +-0.79058E+01 23.125 0.57700E+02 +-0.75960E+01 23.375 0.60062E+02 +-0.77500E+01 23.625 0.55321E+02 +-0.74378E+01 23.875 0.56978E+02 +-0.75484E+01 24.125 0.53835E+02 +-0.73372E+01 24.375 0.55097E+02 +-0.74228E+01 24.625 0.50683E+02 +-0.71192E+01 24.875 0.54050E+02 +-0.73518E+01 25.125 0.52134E+02 +-0.72204E+01 25.375 0.53560E+02 +-0.73185E+01 25.625 0.50013E+02 +-0.70720E+01 25.875 0.49206E+02 +-0.70147E+01 26.125 0.45435E+02 +-0.67406E+01 26.375 0.46474E+02 +-0.68172E+01 26.625 0.43812E+02 +-0.66190E+01 26.875 0.42412E+02 +-0.65124E+01 27.125 0.45641E+02 +-0.67558E+01 27.375 0.41819E+02 +-0.64668E+01 27.625 0.41776E+02 +-0.64634E+01 27.875 0.43219E+02 +-0.65741E+01 28.125 0.39809E+02 +-0.63095E+01 28.375 0.40325E+02 +-0.63502E+01 28.625 0.41312E+02 +-0.64275E+01 28.875 0.40986E+02 +-0.64020E+01 29.125 0.41604E+02 +-0.64501E+01 29.375 0.39131E+02 +-0.62555E+01 29.625 0.37276E+02 +-0.61054E+01 29.875 0.40934E+02 +-0.63980E+01 30.125 0.39131E+02 +-0.62555E+01 30.375 0.38289E+02 +-0.61878E+01 30.625 0.38530E+02 +-0.62072E+01 30.875 0.37550E+02 +-0.61278E+01 31.125 0.38822E+02 +-0.62307E+01 31.375 0.37310E+02 +-0.61082E+01 31.625 0.40479E+02 +-0.63623E+01 31.875 0.34450E+02 +-0.58694E+01 32.125 0.35343E+02 +-0.59450E+01 32.375 0.37508E+02 +-0.61243E+01 32.625 0.36683E+02 +-0.60566E+01 32.875 0.34450E+02 +-0.58694E+01 33.125 0.35824E+02 +-0.59853E+01 33.375 0.36442E+02 +-0.60368E+01 33.625 0.36898E+02 +-0.60743E+01 33.875 0.36958E+02 +-0.60793E+01 34.125 0.33806E+02 +-0.58143E+01 34.375 0.34038E+02 +-0.58342E+01 34.625 0.30267E+02 +-0.55016E+01 34.875 0.33883E+02 +-0.58209E+01 \END; /*===================================================================*/ |