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 /* NRDF D1485 Data No.13                                             */
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 /* Bibliography                                                      */
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 \\BIB,13;
 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);
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 /* Experimental Conditions                                           */
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 \\EXP,13;
 /* 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=30KEV;
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 /* Descriptive Parameters                                            */
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 \\DATA,13;
 INC-ENGY-LAB=30KEV;
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 /* Data Table                                                        */
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 \DATA;
 THTC T22 DELTA-T22'18'
 (DEG) (NODIM) (NODIM)
 1.037E+01 3.368E-03 +-6.544E-03
 2.112E+01 3.602E-03 +-7.853E-03
 3.195E+01 -4.328E-02 +-1.047E-02
 4.197E+01 -6.270E-02 +-1.440E-02
 5.195E+01 -1.285E-01 +-8.052E-03
 6.257E+01 -2.036E-01 +-9.162E-03
 7.261E+01 -2.361E-01 +-1.440E-02
 8.270E+01 -2.961E-01 +-1.178E-02
 9.279E+01 -3.509E-01 +-1.571E-02
 1.032E+02 -3.532E-01 +-1.178E-02
 1.127E+02 -3.151E-01 +-1.571E-02
 1.222E+02 -2.704E-01 +-9.162E-03
 1.324E+02 -1.955E-01 +-1.047E-02
 1.415E+02 -1.521E-01 +-1.571E-02
 1.510E+02 -6.032E-02 +-9.162E-03
 1.609E+02 -1.691E-02 +-9.162E-03
 \END;
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