|
| /*===================================================================*/
/* NRDF D1581 Data No.11 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,11;
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,11;
/* 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=INEL-SCATT;
PHQ=VCTR-ANALPW;
INC-ENGY-LAB=74.72MEV;
DELTA-INC-ENGY-LAB=0.1%;
ANL=CC;
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,11;
INC-ENGY-LAB=74.72MEV;
DELTA-INC-ENGY-LAB=0.1%;
SYS-ERR=5%'36';
/* '36' Total systematic error */
EMT=P;
EXC-ENGY=2.429MEV;
J-PTY=5/2-;
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
TRNSF-MOM-CM AY DELTA-AY
(1/FM) (NODIM) (NODIM)
3.350E-01 -6.897E-02 +-1.552E-01
4.223E-01 -7.471E-02 +-2.011E-01
5.049E-01 1.724E-02 +-9.195E-02
5.874E-01 4.598E-02 +-6.322E-02
6.699E-01 6.897E-02 +-7.471E-02
7.476E-01 4.023E-02 +-4.598E-02
8.350E-01 7.471E-02 +-4.598E-02
9.126E-01 1.034E-01 +-NEGLIGIBLE
9.951E-01 6.897E-02 +-4.023E-02
1.078E+00 5.747E-02 +-NEGLIGIBLE
1.155E+00 5.747E-02 +-NEGLIGIBLE
1.228E+00 5.172E-02 +-NEGLIGIBLE
1.306E+00 2.874E-02 +-NEGLIGIBLE
1.383E+00 -2.299E-02 +-NEGLIGIBLE
1.447E+00 -4.023E-02 +-NEGLIGIBLE
1.451E+00 -7.471E-02 +-NEGLIGIBLE
1.534E+00 -8.046E-02 +-NEGLIGIBLE
1.597E+00 -8.621E-02 +-NEGLIGIBLE
1.602E+00 -1.149E-01 +-NEGLIGIBLE
1.675E+00 -9.770E-02 +-NEGLIGIBLE
1.743E+00 -1.207E-01 +-NEGLIGIBLE
1.811E+00 -1.092E-01 +-NEGLIGIBLE
1.874E+00 -1.034E-01 +-NEGLIGIBLE
1.937E+00 -5.747E-02 +-NEGLIGIBLE
1.937E+00 -9.770E-02 +-NEGLIGIBLE
2.000E+00 -6.322E-02 +-NEGLIGIBLE
2.058E+00 -5.747E-02 +-NEGLIGIBLE
2.126E+00 -8.046E-02 +-NEGLIGIBLE
2.189E+00 -6.322E-02 +-NEGLIGIBLE
2.238E+00 -6.322E-02 +-NEGLIGIBLE
2.296E+00 -9.195E-02 +-NEGLIGIBLE
2.354E+00 -1.092E-01 +-NEGLIGIBLE
2.413E+00 -1.207E-01 +-NEGLIGIBLE
2.466E+00 -1.207E-01 +-NEGLIGIBLE
2.515E+00 -2.299E-02 +-NEGLIGIBLE
2.568E+00 -6.897E-02 +-NEGLIGIBLE
2.617E+00 2.874E-02 +-NEGLIGIBLE
2.660E+00 1.207E-01 +-2.069E-01
2.704E+00 7.471E-02 +-8.046E-02
2.748E+00 1.034E-01 +-4.598E-02
2.801E+00 2.356E-01 +-6.897E-02
\END;
/*===================================================================*/
|