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 /* NRDF D1369 Data No.18                                             */
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 /* Bibliography                                                      */
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 \\BIB,18;
 D#=D1369;
 TITLE=/ Energy dependence of tensor analyzing powers in deuteron
         elastic scattering from 208Pb /;
 ATH=(T.MURAYAMA'1', Y.TAGISHI'1', T.SAKAI'1', M.TOMIZAWA'1',
      H.NISHIKAWA'1', S.SEKI'1');
 INST-ATH=(2JPNTSU'1');
      /* '1' Institute of Physics and Tandem Accelerator Center */
 REF=NP/A;
 VLP=486(1988)261;
 /* Secondary reference 
    - Murayama, Thesis(1987)
 RCTS=208PB(D,D)208PB;
 PHQS=(XSECTN-RATIO, VCTR-ANALPW, TNSR-ANALPW, OPT-POTL-PARA);
 /*===================================================================*/
 /* Experimental Conditions                                           */
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 \\EXP,18;
 /* 2004-11-24 : Converted, N.Otuka + Am. Converted to EXFOR E1369
 RTY=ELA-SCATT;
 ENR=99.86%;
 CHM=ELM;
 PHYS-FORM=SLD;
 THK-TGT=(0.5MG/CM**2,2.3MG/CM**2,7.0MG/CM**2);
 BAC=SELF;
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=VDGT'2';
 /* '2' 12UD Pelletron */
 INST-ACC=2JPNTSU;
 BEAM-INTNSTY=[50NA;
 POL-PRJ=75%'3';
 /* '3' Monitored by quenching method and polarimeter based on
        3He(d,p)4He reaction */
 ION-SOURCE=/ Lamb-shift source /;
 DET-PARTCL=D;
 COINC=NO;
 ANT-COINC=NO;
 DET-SYS=(SBD'4',EDE);
 /* '4' To detect emitted charged particles */
 SOLID-ANGL=3.0MSR;
 ERS-DET=200KEV'5';
 /* '5' Mainly due to target thickness */
 ANL=OPT-MODEL;
 /* 2004-12-14 : Altered, At. Re-digitized */
 /* 2007-03-14 : Altered, N.Otuka. Data replaced by tabulated data
    in thesis */
 RCT=208PB(D,D)208PB;
 PHQ=TNSR-ANALPW;
 INC-ENGY-LAB-RANGE=12MEV;
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 /* Descriptive Parameters                                            */
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 \\DATA,18;
 SYS-ERR=(2%'6',[10%'7');
 /* '6' Uncertainty in beam polarization */
 /* '7' Uncertainty in normalization of cross sections */
 INC-ENGY-LAB=12MEV;
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 /* Data Table                                                        */
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 \DATA;
 THTC T20 DELTA-T20'15'
 (DEG) (NODIM) (NODIM)
 70.52 -0.0038 +-0.0012
 75.53 -0.0033 +-0.0012
 80.54 -0.0040 +-0.0012
 85.55 -0.0034 +-0.0013
 90.55 -0.0056 +-0.0011
 95.55 -0.0008 +-0.0021
 100.54 -0.0052 +-0.0021
 105.53 -0.0029 +-0.0021
 110.52 -0.0036 +-0.0028
 115.50 -0.0055 +-0.0016
 120.48 -0.0053 +-0.0017
 125.45 -0.0046 +-0.0017
 130.42 -0.0055 +-0.0014
 135.39 -0.0033 +-0.0014
 140.35 0.0051 +-0.0014
 145.32 0.0074 +-0.0013
 150.28 0.0112 +-0.0013
 155.23 0.0143 +-0.0021
 160.19 0.0139 +-0.0021
 165.14 0.0161 +-0.0019
 170.10 0.0216 +-0.0020
 \END;
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