| /*===================================================================*/
/* NRDF D1723 Data No.5 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,5;
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,5;
/* 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'26';
/* '26' Axz for deuteron */
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,5;
INC-ENGY-LAB=270MEV;
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
THTC
(DEG) (NODIM) (NODIM)
2.182E+01 -5.656E-03 +-NEGLIGIBLE
2.470E+01 -1.370E-02 +-NEGLIGIBLE
2.824E+01 4.915E-03 +-NEGLIGIBLE
3.145E+01 1.020E-02 +-NEGLIGIBLE
4.428E+01 2.601E-02 +-NEGLIGIBLE
4.718E+01 5.797E-02 +-NEGLIGIBLE
5.071E+01 7.125E-02 +-NEGLIGIBLE
5.200E+01 1.006E-01 +-NEGLIGIBLE
5.521E+01 1.165E-01 +-NEGLIGIBLE
5.746E+01 1.271E-01 +-NEGLIGIBLE
6.068E+01 1.911E-01 +-NEGLIGIBLE
6.229E+01 2.017E-01 +-NEGLIGIBLE
6.583E+01 2.497E-01 +-3.467E-02
1.169E+02 4.143E-01 +-4.267E-02
1.272E+02 4.648E-01 +-2.400E-02
1.304E+02 4.727E-01 +-2.133E-02
1.323E+02 4.940E-01 +-NEGLIGIBLE
1.352E+02 5.020E-01 +-2.401E-02
1.374E+02 5.420E-01 +-NEGLIGIBLE
1.403E+02 5.712E-01 +-2.399E-02
1.435E+02 5.739E-01 +-2.666E-02
1.458E+02 6.352E-01 +-NEGLIGIBLE
1.477E+02 6.751E-01 +-2.933E-02
1.500E+02 7.204E-01 +-2.933E-02
1.516E+02 7.497E-01 +-2.667E-02
1.539E+02 7.924E-01 +-2.933E-02
1.561E+02 8.137E-01 +-3.200E-02
1.580E+02 8.163E-01 +-2.933E-02
1.584E+02 8.616E-01 +-NEGLIGIBLE
1.606E+02 8.776E-01 +-2.934E-02
1.629E+02 8.349E-01 +-NEGLIGIBLE
1.648E+02 7.735E-01 +-2.667E-02
1.670E+02 6.668E-01 +-NEGLIGIBLE
1.689E+02 5.895E-01 +-NEGLIGIBLE
1.711E+02 4.615E-01 +-NEGLIGIBLE
1.730E+02 3.601E-01 +-NEGLIGIBLE
1.781E+02 9.869E-02 +-NEGLIGIBLE
\END;
/*===================================================================*/
|