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 /* NRDF D1485 Data No.1                                              */
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 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,1;
 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                                           */
 /*===================================================================*/
 \\EXP,1;
 /* 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=VCTR-ANALPW;
 INC-ENGY-LAB-RANGE=30KEV;
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 /* Descriptive Parameters                                            */
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 \\DATA,1;
 INC-ENGY-LAB=30KEV;
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 THTC IT11 DELTA-IT11'6'
 (DEG) (NODIM) (NODIM)
 1.057E+01 1.730E-02 +-8.609E-03
 2.070E+01 2.503E-02 +-5.476E-03
 3.114E+01 4.450E-02 +-7.827E-03
 4.187E+01 6.318E-02 +-5.479E-03
 5.142E+01 5.996E-02 +-8.609E-03
 6.160E+01 1.060E-01 +-7.044E-03
 7.206E+01 1.388E-01 +-1.487E-02
 8.220E+01 1.450E-01 +-9.397E-03
 9.203E+01 1.425E-01 +-1.174E-02
 1.022E+02 1.714E-01 +-8.609E-03
 1.120E+02 1.517E-01 +-1.487E-02
 1.221E+02 1.548E-01 +-8.609E-03
 1.319E+02 1.257E-01 +-1.017E-02
 1.421E+02 1.162E-01 +-7.827E-03
 1.513E+02 8.798E-02 +-9.392E-03
 1.617E+02 6.362E-02 +-6.261E-03
 \END;
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