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 /* NRDF D1590 Data No.1                                              */
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 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,1;
 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,1;
 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);
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 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,1;
 INC-ENGY-LAB=270MEV;
 EMT=2HE;
 RSD=12B;
 EXC-ENGY=0MEV;
 J-PTY=1+;
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 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 THTC  DSIGMA/DOMEGA  DELTA-DSIGMA/DOMEGA
 (DEG)   (MB/SR)       (MB/SR)
  4.266E-01  1.381E+00  +0.000E+00-0.000E+00
  1.321E+00  1.219E+00  +0.000E+00-0.000E+00
  2.253E+00  1.057E+00  +0.000E+00-0.000E+00
  3.405E+00  6.560E-01  +0.000E+00-0.000E+00
  4.559E+00  3.906E-01  +0.000E+00-0.000E+00
  5.655E+00  2.496E-01  +0.000E+00-0.000E+00
  6.693E+00  1.632E-01  +0.000E+00-0.000E+00
  7.498E+00  9.257E-02  +0.000E+00-0.000E+00
  8.281E+00  5.633E-02  +0.000E+00-0.000E+00
  9.255E+00  4.473E-02  +0.000E+00-0.000E+00
  1.019E+01  2.365E-02  +0.000E+00-0.000E+00
  1.130E+01  1.741E-02  +0.000E+00-0.000E+00
  1.365E+01  8.000E-03  +1.545E-03-1.545E-03
  1.453E+01  6.500E-03  +1.489E-03-1.489E-03
  1.546E+01  4.053E-03  +6.988E-04-6.988E-04
  1.631E+01  3.838E-03  +1.107E-03-1.107E-03
  1.739E+01  2.600E-03  +1.320E-03-1.320E-03
  1.825E+01  1.424E-03  +1.096E-03-1.096E-03
 \END;
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