/*===================================================================*/ /* NRDF D0357 Data No.20 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,20; D#=D357; TITLE=/APPLICATION OF THE CRYSTAL BLOCKING TECHNIQUE TO THE STUDY OF THE HIGHLY EXCITED NUCLEAR CONTINUUM/; PURPOSE=/TO EXAMINE CHANGES OF THE REACTION TIMES DUE TO ENHANCEMENT OF CERTAIN STATES AMONG THE MANY COMPOUND NUCLEAR FINE-STRUCTURE RESONANCES BY AN ISOBARIC ANALOGUE RESONANCE./; ATH=(W.M.GIBSON'1,2',M.MARUYAMA'3',Y.HASHIMOTO'3',E.P.KANTER'3', G.M.TEMMER'3',R.J.KEDDY'4',D.W.MINGAY'4',J.P.F.SELLSCHOP'4'); INST-ATH=(1USABEL'1',1USAALB'2',1USARUT'3',3SAFWIT'4'); /*@7@*/ REF=NP/A; VLP=317(1979)313; RCTS=(70GE(P,P)70GE,72GE(P,P)72GE,74GE(P,P)74GE); /*===================================================================*/ /* Experimental Conditions */ /*===================================================================*/ \\EXP,20; ENR=NAT; CHM=ELN; THK-TGT=X'1'; /*@8@*/ BAC=C'2'; /*@11@*/ POL-TGT=NO; ACC=(VDG); INST-ACC=1USARUT; INC-ENGY-LAB-RANGE=(5.035MEV,5.110MEV,4.200MEV,3.708MEV,4.358MEV, 5.210MEV); POL-PRJ=NO; DET-PARTCL=(P); DET-SYS=(PS-SI); ERS-DET=58KEV; ANL=(DWBA,STATIST-MODEL,X'1'); /*@9@*/ PHQ=(X'1'); /*@14@*/ /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,20; INC-ENGY-LAB=5.035MEV; CMPD=AS; RSD=GE; EXC-ENGY-EMT=4.0MEV; /*FIG.12*/ /* D357 FIG.12 */ /* SER#= 20 */ /* XSCALE=LINEAR YSCALE=LINEAR */ /* XMAX= 4.00000000E+00 YMAX= 6.99999988E-01 */ /* XMIN= 0.00000000E+00 YMIN= 0.00000000E+00 */ /* FOLLOWING DATA ARE TAKEN FROM GRAPH */ /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; DATA1'1' DATA2'2' DELTA-DATA2 (ANGSTROM) (NODIM) (NODIM) 0.000 9.256E-02 5.785E-03 0.100 1.041E-01 1.012E-02 0.205 1.374E-01 1.301E-02 0.305 1.909E-01 1.012E-02 0.399 2.473E-01 1.157E-02 0.504 2.893E-01 8.677E-03 0.610 3.225E-01 1.012E-02 0.704 3.500E-01 1.446E-02 0.809 3.775E-01 1.301E-02 0.903 3.992E-01 1.012E-02 1.009 4.107E-01 1.157E-02 1.202 4.324E-01 1.157E-02 1.408 4.483E-01 1.446E-02 1.496 4.585E-01 1.301E-02 1.607 4.599E-01 1.012E-02 1.806 4.715E-01 1.157E-02 2.006 4.874E-01 7.231E-03 2.205 5.062E-01 1.157E-02 2.405 5.207E-01 1.301E-02 2.510 5.264E-01 1.012E-02 2.604 5.351E-01 8.677E-03 2.815 5.467E-01 1.446E-02 2.997 5.554E-01 1.590E-02 3.513 5.756E-01 1.012E-02 4.018 6.060E-01 7.231E-03 4.510 6.277E-01 8.677E-03 4.985 6.446E-01 X 5.455 6.619E-01 X 6.041 6.763E-01 X 7.214 7.137E-01 X 8.446 7.367E-01 X 9.795 7.511E-01 X 11.613 7.712E-01 X 13.372 7.827E-01 X 14.956 7.885E-01 X 16.305 7.914E-01 X 18.592 7.971E-01 X \END; /*===================================================================*/ |