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