/*===================================================================*/
 /* NRDF D1723 Data No.3                                              */
 /*===================================================================*/
 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,3;
 D#=D1723;
 TITLE=/ Precise measurement of dp elastic scattering at 270 MeV and
         three-nucleon force effects /;
 PURPOSE=/ To present precise data on the dp cross section and the
           complete set of analyzing powers a_y^d,a_xx,a_yy, anda_z at
           e_d=270MeV spanning nearly the whole angular
           rangetheta(cm)=57deg-138deg. /;
 ATH=(H.SAKAI'1,5', K.SEKIGUCHI'1', H.WITALA'2', W.GLOCKLE'3',
      M.HATANO'1', H.KAMADA'3', H.KATO'1', Y.MAEDA'1', A.NOGGA'3',
      T.OHNISHI'1', H.OKAMURA'4', N.SAKAMOTO'5', S.SAKODA'1',
      Y.SATOU'5', K.SUDA'4', A.TAMII'1', T.UESAKA'4', T.WAKASA'6',
      K.YAKO'1');
 INST-ATH=(2JPNTOK'1', 3POLUJK'2', 2GERBOC'3', 2JPNSUU'4', 2JPNIPC'5',
           2JPNRCN'6');
      /* '1' Department of Physics */
      /* '2' Institute of Physics */
      /* '3' Institute fur Physik II */
      /* '4' Department of Physics */
 REF=PRL;
 VLP=84(2000)5288;
 RCTS=1H(D,D)1H;
 PHQS=(ANGL-DSTRN, VCTR-ANALPW'7', TNSR-ANALPW'8', TNSR-ANALPW'9',
       TNSR-ANALPW'10', POL-TRNSF'11', POL-TRNSF'12', POL'13',
       POL-TRNSF'14');
 /* '7' Ay of Deuteron */
 /* '8' Axx for deuteron */
 /* '9' Ayy for deuteron */
 /* '10' Axz for deuteron */
 /* '11' Tensor-to-vector polarization transfer coefficient K(xx,y')
 /* '12' Tensor-to-vector polarization transfer coefficient K(yy,y')
 /* '13' Induced polarization of outgoing proton P(y') */
 /* '14' Tensor-to-vector polarization transfer coerricient K(xz,y')
 /*===================================================================*/
 /* Experimental Conditions                                           */
 /*===================================================================*/
 \\EXP,3;
 /* 2002-09-26 : Converted, Ay + N.Otuka. Data converted to EXFOR
    E1723 */
 /* 2004-11-25 : Altered, N.Otuka. INSTITUTE, REFERENCE and heading
    of systematic error corrected */
 RTY=ELA-SCATT;
 ENR=X%;
 CHM=CH2;
 PHYS-FORM=SLD;
 THK-TGT=46.7MG/CM**2;
 BAC=X;
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=CYC'15';
 /* '15' Riken Accelerator Research Facility (RARF) */
 INST-ACC=2JPNIPC;
 INC-ENGY-LAB-RANGE=270MEV;
 POL-PRJ=70+-10%;
 DET-PARTCL=(D,P);
 COINC=NO;
 ANT-COINC=NO;
 DET-SYS=MAG'16';
 /* '16' To detect either the scattered proton or deuteron, SMART,
         see [T.Ichihara et al., Nucl.Phys.A569(1994)287c] with
         Focal-plane polarimeter DPOL to measure proton polarization,
         see [S.Ishida et al., AIP Conf.Proc.343(1995)182]. */
 CALB-DET=/ Polarimeter DPOL was primarily designed and optimized for
            deuteron polarization measurements. Therefore the effective
            analyzing power  of DPOL had to be calibrated for
            protons. It was done at 198 MeV by utilizing the induced
            polarization Py /;
 MONTR-RCT=/ , Beam polarization was monitored by using dp scatgtering
             [N.Sakamoto et al., Phys.Lett.B367(1996)60]. /;
 ANL=FADDEEV'17';
 /* '17' See [W.Glockle et al., Phys.Rep.274(1996)107]. */
 /* 2006-08-01 : Altered, T.Ashizawa. Re-digitized */
 /* 2007-03-19 : Altered, N.Otuka. SF7 corrected */
 /* 2007-12-31 : Altered, N.Otuka. SF1 and SF2 swapped, SF7 deleted
 RCT=1H(D,D)1H;
 PHQ=TNSR-ANALPW'22';
 /* '22' Axx for deuteron */
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,3;
 INC-ENGY-LAB=270MEV;
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 THTC
 (DEG) (NODIM) (NODIM)
 1.057E+01 -8.889E-06 +-NEGLIGIBLE
 2.210E+01 -7.734E-02 +-NEGLIGIBLE
 2.530E+01 -9.334E-02 +-NEGLIGIBLE
 2.819E+01 -1.280E-01 +-NEGLIGIBLE
 3.171E+01 -1.627E-01 +-NEGLIGIBLE
 3.523E+01 -1.787E-01 +-NEGLIGIBLE
 3.875E+01 -2.053E-01 +-NEGLIGIBLE
 4.196E+01 -2.613E-01 +-NEGLIGIBLE
 4.420E+01 -2.880E-01 +-NEGLIGIBLE
 4.740E+01 -3.227E-01 +-NEGLIGIBLE
 5.125E+01 -3.840E-01 +-NEGLIGIBLE
 5.221E+01 -3.893E-01 +-NEGLIGIBLE
 5.573E+01 -4.320E-01 +-NEGLIGIBLE
 5.765E+01 -4.533E-01 +-NEGLIGIBLE
 6.117E+01 -4.773E-01 +-NEGLIGIBLE
 6.214E+01 -4.747E-01 +-NEGLIGIBLE
 6.598E+01 -4.907E-01 +-NEGLIGIBLE
 1.169E+02 -3.173E-01 +-3.467E-02
 1.272E+02 -2.800E-01 +-NEGLIGIBLE
 1.300E+02 -2.827E-01 +-NEGLIGIBLE
 1.323E+02 -3.013E-01 +-NEGLIGIBLE
 1.352E+02 -2.880E-01 +-NEGLIGIBLE
 1.371E+02 -2.987E-01 +-NEGLIGIBLE
 1.403E+02 -3.200E-01 +-NEGLIGIBLE
 1.438E+02 -3.547E-01 +-NEGLIGIBLE
 1.457E+02 -3.840E-01 +-NEGLIGIBLE
 1.477E+02 -4.187E-01 +-NEGLIGIBLE
 1.499E+02 -4.667E-01 +-NEGLIGIBLE
 1.515E+02 -4.800E-01 +-NEGLIGIBLE
 1.537E+02 -4.800E-01 +-NEGLIGIBLE
 1.557E+02 -4.773E-01 +-NEGLIGIBLE
 1.582E+02 -4.000E-01 +-NEGLIGIBLE
 1.605E+02 -3.707E-01 +-NEGLIGIBLE
 1.627E+02 -2.773E-01 +-NEGLIGIBLE
 1.646E+02 -1.733E-01 +-NEGLIGIBLE
 1.665E+02 -6.934E-02 +-NEGLIGIBLE
 1.691E+02 2.132E-02 +-NEGLIGIBLE
 1.710E+02 1.120E-01 +-NEGLIGIBLE
 1.730E+02 1.920E-01 +-NEGLIGIBLE
 1.778E+02 3.040E-01 +-NEGLIGIBLE
 \END;
 /*===================================================================*/