/*===================================================================*/ /* NRDF D1590 Data No.4 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,4; D#=D1590; TITLE=/TENSOR ANALYZING POWER OF THE (D,2HE) REACTION AT 270 MEV/; PURPOSE=/IDENTIFYING THE J-PTY OF SPIN-FLIP DIPOLE STATES UTILIZING THE TENSOR ANALYZING POWER./; ATH=(H.OKAMURA'1',S.FUJITA'1',Y.HARA'2',K.HATANAKA'4',T.ICHIHARA'3', S.ISHIDA'1',K.KATOH'2',T.NIIZEKI'2',H.OHNUMA'2',H.OTSU'1', H.SAKAI'1',N.SAKAMOTO'1',Y.SATOU'1',T.UESAKA'1',T.WAKASA'1', T.YAMASHITA'2'); INST-ATH=(2JPNTOK'1',2JPNTIT'2',2JPNIPC'3',2JPNRCN'4'); REF=PL/B; VLP=345(1995)1; RCTS=(12C(D,2HE)12B); PHQS=(ANGL-DSTRN,ANALPW); /*===================================================================*/ /* Experimental Conditions */ /*===================================================================*/ \\EXP,4; RCTS=12C(D,2HE)12B; RTY=(DIRECT-RCT'5');/*@5@*/ ENR=NAT; CHM=ELM; PHYS-FORM=SLD; THK-TGT=9.76MG/CM**2; BAC=SELF; POL-TGT=0%; ALGN-TGT=0%; ACC=(CYC); INST-ACC=2JPNIPC; INC-ENGY-LAB=270MEV; ERS-PRJ=XKEV; BEAM-INTNSTY=0.1NA[2NA; CHRG-INC-ION=1+; POL-PRJ=70%[75%; ION-SOURCE=/REFERENCE: H.OKAMURA ET AL., AIP CONF.PROC.293(1994)84, AND NUCL.PHYS.A577(1994)89C/; DET-PARTCL=P; COINC=YES; ANT-COINC=NO; DET-SYS=(X'8');/*@8@*/ SOLID-ANGL=XMSR; ERS-DET=XKEV; ANL=(DWBA); PHQ=(ANGL-DSTRN); /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,4; INC-ENGY-LAB=270MEV; EMT=2HE; RSD=12B; EXC-ENGY=4.5MEV; J-PTY=(2-,4-); /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; THTC DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA (DEG) (MB/SR) (MB/SR) 3.011E-01 3.607E-01 +0.000E+00-0.000E+00 1.026E+00 4.079E-01 +0.000E+00-0.000E+00 1.961E+00 4.263E-01 +0.000E+00-0.000E+00 3.093E+00 3.695E-01 +0.000E+00-0.000E+00 4.036E+00 3.255E-01 +0.000E+00-0.000E+00 5.424E+00 3.184E-01 +0.000E+00-0.000E+00 6.331E+00 2.788E-01 +0.000E+00-0.000E+00 7.358E+00 2.059E-01 +0.000E+00-0.000E+00 8.258E+00 1.404E-01 +0.000E+00-0.000E+00 9.105E+00 1.308E-01 +0.000E+00-0.000E+00 9.987E+00 8.715E-02 +0.000E+00-0.000E+00 1.123E+01 8.185E-02 +0.000E+00-0.000E+00 1.238E+01 7.384E-02 +0.000E+00-0.000E+00 1.349E+01 5.977E-02 +0.000E+00-0.000E+00 1.465E+01 4.268E-02 +0.000E+00-0.000E+00 1.542E+01 3.113E-02 +0.000E+00-0.000E+00 1.625E+01 2.710E-02 +0.000E+00-0.000E+00 1.719E+01 2.307E-02 +0.000E+00-0.000E+00 1.812E+01 1.419E-02 +0.000E+00-0.000E+00 1.928E+01 1.019E-02 +2.111E-03-2.111E-03 \END; /*===================================================================*/ |