/* 2002-03-18 N.OTUKA 10 POINTS CHECK */ /* 2005-04-19 N.OTUKA PC in DET-SYS replaced by PROP-CNTR */ /* 2005-04-19 N.OTUKA JAP replaced by JPN */ \\BIB,1[6; D#=D352; TITLE=/SYSTEMATIC OBSERVATION OF FINE STRUCTURE OF THE HOLE-STATE ANALOGUES IN NI ISOTOPES/; ATH=(H.IKEGAMI'1',T.YAMAZAKI'1',S.MORINOBU'1',I.KATAYAMA'1', M.FUJIWARA'1',Y.FUJITA'1',H.TAKETANI'2',M.ADACHI'2', T.MATSUZAKI'2',K.KOORI'3',M.MATOBA'3'); INST-ATH=(2JPNRCN'1',2JPNINS'2',2JPNKYU'3'); REF=NP/A; VLP=329(1979)84; RCTS=(58NI(P,D)57NI,62NI(P,D)61NI,64NI(P,D)63NI); \\EXP,1[6; ENR=%; CHM=ELM; THK-TGT=XMG/CM**2'54'; /*@54@*/ BAC=SELF; POL-TGT=NO; ALGN-TGT=NO; ACC=(CYC'52'); /*@52@*/ INST-ACC=2JPNRCN; INC-ENGY-RANGE=(50MEV); DELTA-INC-ENGY=XKEV; BEAM-INTNSTY=20NA; POL-PRJ=NO; DET-PARTCL=(D); DET-SYS=(MAG+PS-PC+PLST-SCT'53',PROP-CNTR); /*@53@*/ SOLID-ANGL=3.4MSR; ERS-DET=XKEV'55'; /*@55@*/ PHQ=(XSECTN,ANGL-DSTRN,ENGY-SPEC,DSIGMA/DOMEGA,IAS,TRNSF-L); \\EXP,1[3; RCT=58NI(P,D)57NI; PHQ=(DSIGMA/DOMEGA,EXC-ENGY,IAS,TRNSF-L); \\DATA,1; INC-ENGY-LAB=50MEV; EXC-ENGY=5.132MEV; TRNSF-L=3; /*FIG.3-(A)*/ /* D352 FIG.3-(A) */ /* SER#= 1 */ /* XSCALE=LINEAR YSCALE=LOG */ /* XMAX= 5.00000000E+01 YMAX= 2.99999952E-01 */ /* XMIN= 1.00000000E+01 YMIN= 5.99999987E-02 */ /* FOLLOWING DATA ARE TAKEN FROM GRAPH */ \DATA; THTC DSIGMA/DOMEGA DELTA-DSIGMA-DOMEGA (DEG) (MB/SR) (MB/SR) 8.227 1.724E-01 1.503E-02 11.330 1.505E-01 1.312E-02 14.765 1.234E-01 7.985E-03 17.535 1.706E-01 1.487E-02 20.748 1.505E-01 1.484E-02 23.850 1.209E-01 1.191E-02 26.842 9.704E-02 1.068E-02 31.053 5.461E-02 5.386E-03 36.260 4.525E-02 3.945E-03 41.136 4.385E-02 5.342E-03 \END; \\DATA,2; INC-ENGY-LAB=50MEV; EXC-ENGY=5.230MEV'21'; J-PI=7/2-; TRNSF-L=3; /*@21@*/ /*FIG.3-(B)*/ /* D352 FIG.3-(B) */ /* SER#= 2 */ /* XSCALE=LINEAR YSCALE=LOG */ /* XMAX= 5.00000000E+01 YMAX= 3.00000000E+00 */ /* XMIN= 1.00000000E+01 YMIN= 1.00000000E+00 */ /* FOLLOWING DATA ARE TAKEN FROM GRAPH */ \DATA; THTC DSIGMA/DOMEGA (DEG) (MB/SR) 8.232 3.262E+00 11.215 3.032E+00 14.420 2.434E+00 17.735 2.759E+00 20.608 2.817E+00 23.702 2.538E+00 26.906 1.954E+00 30.884 1.195E+00 36.298 9.691E-01 41.271 9.793E-01 \END; \\DATA,3; INC-ENGY-LAB=50MEV; EXC-ENGY=5.358MEV; TRNSF-L=3; /*FIG.3-(C)*/ /* D352 FIG.3-(C) */ /* SER#= 3 */ /* XSCALE=LINEAR YSCALE=LOG */ /* XMAX= 5.00000000E+01 YMAX= 2.99999952E-01 */ /* XMIN= 1.00000000E+01 YMIN= 9.99999642E-02 */ /* FOLLOWING DATA ARE TAKEN FROM GRAPH */ \DATA; THTC DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA (DEG) (MB/SR) (MB/SR) 8.011 3.262E-01 2.478E-02 11.326 2.788E-01 2.118E-02 14.641 2.408E-01 2.102E-02 17.735 3.262E-01 2.478E-02 20.939 3.401E-01 2.584E-02 23.702 3.000E-01 2.619E-02 27.127 2.102E-01 2.318E-02 30.994 1.299E-01 1.282E-02 36.298 1.076E-01 1.062E-02 41.271 9.896E-02 9.771E-03 \END; \\EXP,4,5; /*@1@*/ /*@2@*/ /*@3@*/ /*@4@*/ \\EXP,4; RCT=58NI(P,D)57NI; \\DATA,4; CMPD=59CU; RSD=57NI; \DATA; DATA1'1' DATA1-ERR DATA2'2' DATA2-ERR DATA3'3' DATA3-ERR DATA4'4' DATA4-ERR (KEV) (KEV) (PERCENT) (PERCENT) (KV) (KEV) (KEV) (KEV) -99 3 5.5 0.2 -100 3 22.8 0.8 0 0 100 0 0 0 X X 127 3 10.0 0.3 110 3 36.4 0.9 \END; /*@1@*/ /*@2@*/ /*@3@*/ /*@4@*/ \\EXP,5; RCT=60NI(P,D)59NI'22'; /*@22@*/ \\DATA,5; CMPD=61CU; RSD=59NI; \DATA; DATA1'1' DATA1-ERR DATA2'2' DATA2-ERR DATA3'3' DATA3-ERR DATA4'4' DATA4-ERR (KEV) (KEV) (PERCENT) (PERCENT) (KEV) (KEV) (KEV) (KEV) -36.2 0.2 11.0 0.7 -35.8 0.5 10.7 0.3 0 0 100 0 0 0 X X 17.7 0.3 12.2 0.5 12.9 0.4 6.3 0.2 40.1 0.3 14.0 0.9 33.4 0.6 11.6 0.3 \END; /*@1@*/ /*@2@*/ /*@3@*/ /*@4@*/ \\EXP,6; /*@1@*/ /*@5@*/ /*@6@*/ \\DATA,6; \DATA; A DATA1'1' DATA5'5,7' DATA5'5,8' DATA6'6,9' DATA6-ERR DATA6'6,10' (NODIM) (MEV) (MEV) (MEV) (KEV) (KEV) (KEV) 57 5.230 7.36 10.26 [25 X 12 59 7.341 8.61 9.00 [16 X 10 61 9.558 9.86 7.82 9.0 2.0 9 63 11.850 11.28 6.84 9.0 2.0 9 \END; \\END; /*@1@*/ /*@5@*/ /*@7@*/ /*@6@*/ /*@8@*/ /*@9@*/ /*@10@*/ @@52; AVF CYCLOTRON, WHICH WAS ANALYED BY A TANDEM MONOCHROMATOR SYSTEM FORMED BY TWO IDENTICAL ANALYZING MAGNETS DEFLECTED BY A CLEANING MAGNET, ANG THEN FOCUSSED ONTO THE TARGET. THE OTHER BEAM-LINE ELEMENTS WERE TUNED SO AS TO OBTAIN THE REQUIRED BEAM SPOT SIZE AT THE TARGET. @@53; THIS OPERATES IN A THREE-FOLD COINCIDENCE MODE. @@54; SELF-SUPPORTING METALLIC FOIL TARGETS OF ENRICHED NI ISOTOPES (58NI, 700 UG/CM**2; 62NI, 491 UG/CM**2; 64NI, 473 UG/CM**2). @@55; ABOUT 6KEV AND 8-15KEV IN FWHM FOR ELASTICALLY SCATTERED PROTONS AND FOR DEUTERONS FROM (P,D) REACTIONS, RESPECTIVELY. @@21; ISOBARIC ANALOGUE STATE @@1; '1' DATA1= OBSERVED ENERGY SPACINGS OF THE T(UPPER) AND T(LOWER) ISO- SPIN STATES. @@2; '2' DATA2= CROSS-SECTION ROTIONS FOR THE T(UPPER) TO T(LOWER) STATES. @@3; '3' DATA3= UNPERTURBED ENERGY SPACINGS OF THE STATES OF GOOD ISOSPIN. @@4; '4' DATA4= MATRIX ELEMENTS FOR THE ISOSPIN MIXING. @@22; THE RESULTS FROM H.IKEGAMI ET AL., PHYS.LETT. 74B,326,(1978),ARE ALSO SHOWN FOR COMPLETENESS. @@5; '5' DATA5= SEPARTION ENERGY @@6; '6' DATA6= SPREADING WIDTH @@7; '7' FOR PROTON @@8; '8' FOR NEUTRON @@9; '6' EXPERIMENT @@10; '10' CALCULATION @@;