/*===================================================================*/
 /* NRDF D1804 Data No.5                                              */
 /*===================================================================*/
 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,5;
 D#=D1804;
 TITLE=/ Model-independent spin-parity determination by the (d,2He)
         reaction and possible evidence for a 0- state in 12B /;
 ATH=(H.OKAMURA'1', T.UESAKA'1', K.SUDA'1', H.KUMASAKA'1', R.SUZUKI'1',
      A.TAMII'1', N.SAKAMOTO'2', H.SAKAI'2,3');
 INST-ATH=(2JPNSUU'1', 2JPNTOK'2', 2JPNIPC'3');
      /* '1' Department of Physics */
      /* '2' Department of Physics */
 REF=PR/C;
 VLP=66(2002)054602;
 RCTS=12C(D,2HE)12B;
 PHQS=(ENGY-SPEC, TNSR-ANALPW'4', TNSR-ANALPW'5');
 /* '4' Azz */
 /* '5' Ayy */
 /*===================================================================*/
 /* Experimental Conditions                                           */
 /*===================================================================*/
 \\EXP,5;
 /* 2004-08-06 : Compiled+Checked, St + Nk */
 /* 2009-08-23 : Altered, Nf. 004-008 corrected */
 /* Related references 
    - H.Okamura et al., NIM/A, 406(1998)78.
    (Details of detector system and analysis procedure)
 RTY=RRG-RCT'6';
 /* '6' charge-exchange reaction */
 ENR=X%;
 CHM=ELM;
 PHYS-FORM=SLD;
 THK-TGT=10MG/CM**2;
 BAC=X;
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=CYC'7';
 /* '7' Isochronous cyclotron, AVF and ring cyclotron of RIKEN
        accelerator research facility */
 INST-ACC=2JPNIPC;
 INC-ENGY-LAB-RANGE=270MEV;
 BEAM-INTNSTY=[0.4NA;
 ION-SOURCE=/ Polarized ion source (See [H. Okamura et al., in
              Polarized Ion Sources and Polarized Gas Targets, edited
              by L. W. Anderson and W. Haeberili, AIP Conf. Proc. No.
              293 (AIP, New York, 1994), p.84] for detail. Field
              strength and rotation angle of Wien filter were tuned so
              that beam direction is in parallel with polarization
              axis.) /;
 DET-PARTCL=P;
 COINC=(P,P);
 ANT-COINC=NO;
 DET-SYS=(MAG'8',MWDC'9',SCT'10');
 /* '8' SMART [T.Ichihara et al., Nucl. Phys. A569(1994)287c]. To
        analyze momenta of protons emittied from 2He. */
 /* '9' To detect protons */
 /* '10' To detect protons */
 /* Analysis:
    - Integration of energy distribution (Azz values is deduced by
      using Eq.(4) in the reference. Angular distribution appearing in
      this equation is obtained by integrating double differential
      cross section shown in panel Fig.1(a) over excitation energy.)
 /* 2009-08-23 : Altered, Nf. SF5: NN -> LL */
 RCT=12C(D,2HE)12B;
 PHQ=TNSR-ANALPW'27';
 /* '27' Azz */
 POL-PRJ=X%'28';
 /* '28' Results from three tensor polalized beams pzz=-1.16,
         +0.79 and 0 are used to deduce Azz. */
 ANL=CCBA'29';
 /* '29' adiabatic coupled-channel Born approximation [H.Okamura,
         Phys. Rev. C 60(1999)064602]. */
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,5;
 INC-ENGY-LAB=270MEV;
 EXC-ENGY=0MEV;
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 THTC AZZ DELTA-AZZ'30'
 (DEG) (NODIM) (NODIM)
 0.667 0.0921 +-0.0146
 1.556 0.0618 +-0.0103
 2.533 0.0088 +-0.0117
 \END;
 /*===================================================================*/