/*===================================================================*/ /* NRDF D1100 Data No.31 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,31; D#=D1100; TITLE=/EVIDENCE OF A SHAPE TRANSITION IN EVEN-A GE ISOTOPES/; PURPOSE=/TO INVESTIGATE THE COLLECTIVE PROPERTIES OF THE EVEN-EVEN ISOTOPES OF GE(70,72,74,76) AS MANIFESTED IN THE ELASTIC AND INELASTIC SCATTERING TO THE FIRST 2+ STATE OF VECTOR POLARIZED DEUTERONS AND PROTONS FROM THESE NUCLEI./; ATH=(S.SEN'1',S.E.DARDEN'1',R.C.LUHN'1',N.O.GAISER'1',G.MURILLO'2', J.RAMIREZ'2'); INST-ATH=(1USANOT'1',3MEXCNM'2'); REF=PR/C; VLP=31(1985)787; RCTS=(70GE(D,D)70GE,72GE(D,D)72GE,74GE(D,D)74GE,76GE(D,D)76GE, 70GE(P,P)70GE,72GE(P,P)72GE,74GE(P,P)74GE,76GE(P,P)76GE); PHQS=(ANGL-DSTRN,XSECTN-RATIO,ANALPW); /*===================================================================*/ /* Experimental Conditions */ /*===================================================================*/ \\EXP,31; RCT=70GE(P,P)70GE; RTY=(ELA-SCATT,INEL-SCATT); ENR=84.6%; CHM=ELM; THK-TGT=300[350UG/CM**2; BAC=SELF; ACC=(VDGT); INST-ACC=1USANOT; INC-ENGY-LAB=(11.5MEV); BEAM-INTNSTY=7NA; POL-PRJ=0.60'23'; /*@23@*/ DET-PARTCL=(P); DET-SYS=(SSD); ANL=(CC); PHQ=(ANGL-DSTRN,XSECTN-RATIO,ANALPW); /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,31; INC-ENGY-LAB=11.5MEV; EXC-ENGY=1.040MEV; J-PI=2+; /*FIG.8-A*/ /* D1100 FIG.8-(A) */ /* FOLLOWING DATA ARE TAKEN FROM GRAPH */ /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; THTC ANALPW DELTA-ANALPW (DEG) (NODIM) (NODIM) 26.027 -2.716E-02 +1.975E-02-1.481E-02 30.548 -5.926E-02 +1.728E-02-1.728E-02 36.712 -9.136E-02 +1.728E-02-1.728E-02 40.411 -1.506E-01 +2.222E-02-2.222E-02 51.096 -2.420E-01 +1.975E-02-1.728E-02 56.849 -2.593E-01 +2.222E-02-1.975E-02 60.959 -2.272E-01 +1.975E-02-1.728E-02 65.890 -1.556E-01 +2.222E-02-2.222E-02 70.822 -3.210E-02 +2.469E-02-2.469E-02 79.863 8.642E-02 +2.963E-02-1.975E-02 95.890 -1.136E-01 +2.963E-02-2.222E-02 99.589 -2.074E-01 +2.716E-02-2.716E-02 105.342 -2.123E-01 +2.963E-02-2.469E-02 110.274 -2.568E-01 +3.210E-02-2.963E-02 115.616 -2.543E-01 +2.963E-02-2.469E-02 120.137 -1.852E-01 +2.469E-02-1.975E-02 125.479 -5.926E-02 +2.469E-02-2.222E-02 130.000 3.210E-02 +3.951E-02-3.210E-02 140.274 6.667E-02 +3.951E-02-4.198E-02 145.205 1.457E-01 +5.185E-02-4.938E-02 150.959 1.877E-01 +3.951E-02-4.938E-02 154.658 2.765E-01 +5.185E-02-5.432E-02 160.411 3.654E-01 +3.704E-02-3.457E-02 164.932 3.506E-01 +4.444E-02-4.444E-02 \END; /*===================================================================*/ |