/*===================================================================*/
 /* NRDF D1581 Data No.9                                              */
 /*===================================================================*/
 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,9;
 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,9;
 /* 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=74.72MEV;
 DELTA-INC-ENGY-LAB=0.1%;
 ANL=CC;
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,9;
 INC-ENGY-LAB=74.72MEV;
 DELTA-INC-ENGY-LAB=0.1%;
 SYS-ERR=X%'34';
 /* '34' 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 (5.5%) */
 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)
 3.254E-01 2.100E+00 +-NEGLIGIBLE
 4.095E-01 2.558E+00 +-NEGLIGIBLE
 4.937E-01 3.647E+00 +-NEGLIGIBLE
 5.832E-01 5.200E+00 +-NEGLIGIBLE
 6.619E-01 5.517E+00 +-NEGLIGIBLE
 7.460E-01 6.588E+00 +-NEGLIGIBLE
 8.299E-01 6.459E+00 +-NEGLIGIBLE
 9.084E-01 5.739E+00 +-NEGLIGIBLE
 9.871E-01 5.627E+00 +-NEGLIGIBLE
 1.066E+00 4.712E+00 +-NEGLIGIBLE
 1.144E+00 4.025E+00 +-NEGLIGIBLE
 1.222E+00 3.177E+00 +-NEGLIGIBLE
 1.301E+00 2.459E+00 +-NEGLIGIBLE
 1.374E+00 1.794E+00 +-NEGLIGIBLE
 1.452E+00 1.309E+00 +-NEGLIGIBLE
 1.525E+00 1.033E+00 +-NEGLIGIBLE
 1.604E+00 8.156E-01 +-NEGLIGIBLE
 1.667E+00 6.831E-01 +-NEGLIGIBLE
 1.740E+00 5.721E-01 +-NEGLIGIBLE
 1.808E+00 4.697E-01 +-NEGLIGIBLE
 1.871E+00 4.012E-01 +-NEGLIGIBLE
 1.928E+00 3.636E-01 +-5.378E-02
 1.996E+00 2.652E-01 +-NEGLIGIBLE
 2.059E+00 2.178E-01 +-NEGLIGIBLE
 2.116E+00 1.686E-01 +-NEGLIGIBLE
 2.179E+00 1.254E-01 +-NEGLIGIBLE
 2.231E+00 9.151E-02 +-NEGLIGIBLE
 2.288E+00 6.418E-02 +-NEGLIGIBLE
 2.346E+00 4.968E-02 +-NEGLIGIBLE
 2.403E+00 3.349E-02 +-NEGLIGIBLE
 2.450E+00 2.444E-02 +-NEGLIGIBLE
 2.502E+00 1.748E-02 +-NEGLIGIBLE
 2.554E+00 1.250E-02 +-NEGLIGIBLE
 2.596E+00 1.089E-02 +-NEGLIGIBLE
 2.643E+00 7.640E-03 +-NEGLIGIBLE
 2.685E+00 7.947E-03 +-NEGLIGIBLE
 2.727E+00 6.923E-03 +-NEGLIGIBLE
 2.779E+00 5.574E-03 +-NEGLIGIBLE
 \END;
 /*===================================================================*/