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 /* NRDF D1485 Data No.16                                             */
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 /* Bibliography                                                      */
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 \\BIB,16;
 D#=D1485;
 TITLE=/ Analyzing powers for 2H(d,p)3H at incident energies of 30,
         50, 70 and 90 keV /;
 PURPOSE=/ To report measurements of all four analyzing powers,
           iT11,T20, T21 and T22 /;
 ATH=(Y.TAGISHI'1', N.NAKAMOTO'1', K.KATOH'1', J.TOGAWA'1',
      T.HISAMUNE'1', T.YOSHIDA'1', Y.AOKI'1');
 INST-ATH=(2JPNTSU'1');
      /* '1' Institute of Physics and Tandem Accelerator Center */
 REF=PR/C;
 VLP=46(1992)1155;
 RCTS=2H(D,P)3H;
 PHQS=(VCTR-ANALPW, TNSR-ANALPW);
 /*===================================================================*/
 /* Experimental Conditions                                           */
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 \\EXP,16;
 /* 2005-11-25 : Converted, N.Otuka + C.Kurokawa. Converted to
    EXFOR E1485 */
 CHM=X'2';
 /* '2' Parapolyphenyl (C6D4)n */
 PHYS-FORM=SLD;
 THK-TGT=0.0007[0.0012MG/CM**2;
 BAC=C'3';
 /* '3' Al (5-micro meter thick) is also used. */
 THK-BAC=0.02MG/CM**2;
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=VDGT;
 INST-ACC=2JPNTSU;
 BEAM-INTNSTY=50NA;
 POL-PRJ=85%;
 ION-SOURCE=/ Lamb-shift source /;
 DET-PARTCL=P;
 COINC=NO;
 ANT-COINC=NO;
 DET-SYS=(PROP-CNTR'4',SI'5');
 /* '4' Used as proton detector */
 /* '5' Used for T(20) measurement near 180 deg */
 SOLID-ANGL=23MSR;
 ANL=LEGD;
 /* 2006-03-30 : Altered, At. Re-digitized */
 RCT=2H(D,P)3H;
 PHQ=TNSR-ANALPW;
 INC-ENGY-LAB-RANGE=90KEV;
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 /* Descriptive Parameters                                            */
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 \\DATA,16;
 INC-ENGY-LAB=90KEV;
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 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 THTC T22 DELTA-T22'21'
 (DEG) (NODIM) (NODIM)
 9.618E+00 -1.105E-03 +-3.947E-03
 2.039E+01 -1.403E-02 +-5.263E-03
 3.082E+01 -5.064E-02 +-6.579E-03
 4.123E+01 -7.410E-02 +-6.579E-03
 5.168E+01 -1.212E-01 +-3.947E-03
 6.208E+01 -1.434E-01 +-9.210E-03
 7.216E+01 -1.971E-01 +-9.210E-03
 8.257E+01 -2.237E-01 +-1.444E-02
 9.259E+01 -2.484E-01 +-1.050E-02
 1.026E+02 -2.399E-01 +-1.668E-02
 1.125E+02 -2.094E-01 +-1.053E-02
 1.220E+02 -1.842E-01 +-7.894E-03
 1.312E+02 -1.366E-01 +-6.579E-03
 1.410E+02 -7.980E-02 +-9.210E-03
 1.502E+02 -4.934E-02 +-6.579E-03
 1.601E+02 -8.332E-03 +-7.894E-03
 \END;
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