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