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| /*===================================================================*/
/* NRDF D1581 Data No.2 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,2;
D#=D1581;
TITLE=/ Proton scattering off 9Be and the final-state interaction in
the (e,e'p) and (gamma,p) reactions on 10B /;
PURPOSE=/ To study the effect of alternative descriptions of the
final-state interaction on (e,e'p) and (gamma,p) cross
sections on 10B /;
ATH=(L.J.DE BEVER'1', H.P.BLOK'1,2', J.BLOUW'1', M.FUJIWARA'3',
K.HOSONO'3', J.J.KELLY'4', S.KUWAMOTO'5', L.LAPIKAS'1',
G.VAN DER STEENHOVEN'1', K.TAKAHISA'3', J.TAKAMATSU'6',
M.YOSOI'5');
INST-ATH=(2NEDIKO'1', 2NEDFUL'2', 2JPNRCN'3', 1USAMRY'4', 2JPNKTO'5',
2JPNTOH'6');
/* '2' Department of Physics and Astronomy */
/* '4' Department of Physics */
/* '5' Department of Physics */
/* '6' Department of Physics */
REF=NP/A;
VLP=579(1994)13;
RCTS=9BE(P,P)9BE;
PHQS=(OPT-POTL-PARA'7', ANGL-DSTRN, VCTR-ANALPW, OPT-POTL-PARA'8',
OPT-POTL-PARA'9');
/* '7' Optical model parameters resulting from the best fit
searches in the spherical optical model analysis */
/* '8' Optical model parameters resulting from the spherical
optical model analysis after the geometriacal parameters had been
fixed */
/* '9' Optical model parameters resulting from the reduced coupled
channel analysis with quadrupole deformation parameter 0.75 */
/*===================================================================*/
/* Experimental Conditions */
/*===================================================================*/
\\EXP,2;
/* 2005-09-28 : Converted, Converted to EXFOR E1581 */
/* 2005-11-17 : Altered, At + Sr. Re-digitized */
ENR=NAT;
CHM=ELM;
PHYS-FORM=SLD;
THK-TGT=(1.31MG/CM**2, 4.06MG/CM**2, 48.4MG/CM**2)'10';
/* '10' 1.31(4), 4.06(9) and 48.4(5) mg/cm**2 */
POL-TGT=0%;
ALGN-TGT=0%;
ACC=CYC'11';
/* '11' Isochronous cyclotron, AVF cyclotron */
INST-ACC=2JPNRCN;
BEAM-INTNSTY=0.5[6NA;
POL-PRJ=75[80%;
ION-SOURCE=/ Atomic beam source /;
DET-PARTCL=P;
COINC=NO;
ANT-COINC=NO;
DET-SYS=(MAG'12',PROP-CNTR'12',SCT'12',EDE'13');
/* '12' Detection system of RAIDEN consists of gas proportional
counter and plastic scintillator */
/* '13' Plastic scintillator (E) and gas proportional counter
(Delta E) */
SOLID-ANGL=0.82[2.56MSR'14';
/* '14' 0.82(2) msr at forward scattering angles and 2.56(3) msr
at backward scattering angles */
/* Experimental Method:
- Particle identification by 'E/Delta E' measurement (Plastic
scintillator (E) and gas proportional counter (Delta E))
- Beam current integrated (Absolute accuracy of the charge
integration of about 3%)
RCT=9BE(P,P)9BE;
RTY=ELA-SCATT;
PHQ=ANGL-DSTRN;
INC-ENGY-LAB=54.70MEV;
DELTA-INC-ENGY-LAB=0.1%;
ANL=(OPT-MODEL,CC);
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,2;
INC-ENGY-LAB=54.70MEV;
DELTA-INC-ENGY-LAB=0.1%;
SYS-ERR=(4.5[5.0%'17',3.0%'18',1.0[2.0%'19',2.0[3.0%'20',0.0[2.0%'21');
/* '17' Total systematic error. See Table 1, p17 for detail (5.0%
and 4.5% for forward and backward angles) */
/* '18' Uncertainty in charge integration */
/* '19' Uncertainty in solid angle (2.0% and 1.0% for forward and
backward angle) */
/* '20' Uncertainty in target thickness (3.0% and 2.0% for
forward and backward angle) */
/* '21' Uncertainty in target angle (about 0.0% and 2.0% for
forward and backward angle) */
EMT=P;
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
TRNSF-MOM-CM XSECTN-RATIO
(1/FM) (NODIM)
2.875E-01 5.229E+00
3.578E-01 1.169E+01
4.232E-01 2.091E+01
5.040E-01 3.127E+01
5.681E-01 3.915E+01
6.427E-01 4.631E+01
7.067E-01 5.101E+01
7.665E-01 4.605E+01
8.415E-01 4.095E+01
9.100E-01 3.373E+01
9.796E-01 2.804E+01
1.045E+00 2.122E+01
1.107E+00 1.622E+01
1.169E+00 1.357E+01
1.231E+00 1.246E+01
1.302E+00 1.295E+01
1.361E+00 1.423E+01
1.425E+00 1.563E+01
1.484E+00 1.717E+01
1.548E+00 1.799E+01
1.602E+00 1.799E+01
1.660E+00 1.757E+01
1.712E+00 1.728E+01
1.762E+00 1.526E+01
1.810E+00 1.423E+01
1.864E+00 1.295E+01
1.918E+00 1.179E+01
1.966E+00 1.048E+01
2.019E+00 9.321E+00
2.068E+00 8.094E+00
2.110E+00 7.028E+00
2.159E+00 6.708E+00
2.206E+00 6.554E+00
2.244E+00 5.555E+00
2.282E+00 5.304E+00
2.325E+00 5.058E+00
2.368E+00 4.605E+00
2.405E+00 4.097E+00
\END;
/*===================================================================*/
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