/*===================================================================*/
 /* NRDF D1581 Data No.8                                              */
 /*===================================================================*/
 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,8;
 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,8;
 /* 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=ANGL-DSTRN;
 INC-ENGY-LAB=54.70MEV;
 DELTA-INC-ENGY-LAB=0.1%;
 ANL=CC;
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,8;
 INC-ENGY-LAB=54.70MEV;
 DELTA-INC-ENGY-LAB=0.1%;
 SYS-ERR=X%'33';
 /* '33' Total systematic error. Total systematic uncertainty
         (mainly due to charge integration, solid angle, target
         thickness and target angle) estimated to be comparable to that
         in the elastic cross section (4.5-5.0%) */
 EMT=P;
 EXC-ENGY=2.429MEV;
 J-PTY=5/2-;
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 TRNSF-MOM-CM DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA
 (1/FM) (MB/SR) (MB/SR)
 2.790E-01 2.270E+00 +-NEGLIGIBLE
 3.489E-01 2.832E+00 +-NEGLIGIBLE
 4.239E-01 3.907E+00 +-NEGLIGIBLE
 4.964E-01 4.814E+00 +-NEGLIGIBLE
 5.632E-01 5.457E+00 +-NEGLIGIBLE
 6.300E-01 6.316E+00 +-NEGLIGIBLE
 7.022E-01 6.586E+00 +-NEGLIGIBLE
 7.745E-01 7.159E+00 +-NEGLIGIBLE
 8.356E-01 6.725E+00 +-NEGLIGIBLE
 9.022E-01 6.586E+00 +-NEGLIGIBLE
 9.744E-01 6.186E+00 +-9.738E-01
 1.035E+00 5.234E+00 +-NEGLIGIBLE
 1.102E+00 4.522E+00 +-NEGLIGIBLE
 1.163E+00 3.670E+00 +-NEGLIGIBLE
 1.229E+00 2.916E+00 +-NEGLIGIBLE
 1.290E+00 2.270E+00 +-NEGLIGIBLE
 1.356E+00 1.767E+00 +-NEGLIGIBLE
 1.423E+00 1.375E+00 +-NEGLIGIBLE
 1.478E+00 1.116E+00 +-NEGLIGIBLE
 1.534E+00 9.056E-01 +-NEGLIGIBLE
 1.589E+00 7.349E-01 +-NEGLIGIBLE
 1.644E+00 6.620E-01 +-NEGLIGIBLE
 1.700E+00 5.486E-01 +-NEGLIGIBLE
 1.755E+00 4.942E-01 +-NEGLIGIBLE
 1.805E+00 4.270E-01 +-NEGLIGIBLE
 1.855E+00 3.613E-01 +-NEGLIGIBLE
 1.905E+00 3.121E-01 +-NEGLIGIBLE
 1.955E+00 2.586E-01 +-NEGLIGIBLE
 1.999E+00 2.143E-01 +-NEGLIGIBLE
 2.043E+00 1.668E-01 +-NEGLIGIBLE
 2.098E+00 1.271E-01 +-NEGLIGIBLE
 2.137E+00 1.076E-01 +-NEGLIGIBLE
 2.181E+00 8.373E-02 +-NEGLIGIBLE
 2.225E+00 6.655E-02 +-NEGLIGIBLE
 2.259E+00 5.514E-02 +-NEGLIGIBLE
 2.308E+00 4.031E-02 +-NEGLIGIBLE
 2.336E+00 3.556E-02 +-NEGLIGIBLE
 2.369E+00 2.947E-02 +-NEGLIGIBLE
 \END;
 /*===================================================================*/