/*===================================================================*/ /* 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; /*===================================================================*/ |