/*===================================================================*/ /* NRDF D1581 Data No.4 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,4; 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,4; /* 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=VCTR-ANALPW; INC-ENGY-LAB=54.70MEV; DELTA-INC-ENGY-LAB=0.1%; ANL=(OPT-MODEL,CC); /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,4; INC-ENGY-LAB=54.70MEV; DELTA-INC-ENGY-LAB=0.1%; SYS-ERR=3%'27'; /* '27' Total systematic error */ EMT=P; /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; TRNSF-MOM-CM AY DELTA-AY (1/FM) (NODIM) (NODIM) 2.909E-01 8.871E-02 +-NEGLIGIBLE 3.636E-01 6.452E-02 +-NEGLIGIBLE 4.303E-01 4.839E-02 +-NEGLIGIBLE 5.030E-01 7.258E-02 +-NEGLIGIBLE 5.697E-01 5.645E-02 +-NEGLIGIBLE 6.424E-01 5.645E-02 +-NEGLIGIBLE 7.091E-01 5.645E-02 +-NEGLIGIBLE 7.818E-01 4.839E-02 +-NEGLIGIBLE 8.485E-01 4.839E-02 +-NEGLIGIBLE 9.152E-01 4.032E-02 +-NEGLIGIBLE 9.758E-01 4.032E-02 +-6.452E-02 1.048E+00 8.065E-02 +-NEGLIGIBLE 1.109E+00 1.935E-01 +-NEGLIGIBLE 1.176E+00 3.306E-01 +-NEGLIGIBLE 1.242E+00 4.839E-01 +-NEGLIGIBLE 1.303E+00 6.048E-01 +-NEGLIGIBLE 1.370E+00 6.371E-01 +-NEGLIGIBLE 1.424E+00 6.532E-01 +-NEGLIGIBLE 1.491E+00 6.371E-01 +-NEGLIGIBLE 1.545E+00 5.968E-01 +-NEGLIGIBLE 1.606E+00 5.565E-01 +-NEGLIGIBLE 1.655E+00 5.242E-01 +-NEGLIGIBLE 1.709E+00 4.597E-01 +-NEGLIGIBLE 1.770E+00 4.194E-01 +-NEGLIGIBLE 1.824E+00 3.629E-01 +-NEGLIGIBLE 1.879E+00 3.145E-01 +-NEGLIGIBLE 1.933E+00 2.500E-01 +-NEGLIGIBLE 1.976E+00 2.016E-01 +-NEGLIGIBLE 2.024E+00 1.532E-01 +-NEGLIGIBLE 2.073E+00 8.871E-02 +-NEGLIGIBLE 2.121E+00 0.000E+00 +-NEGLIGIBLE 2.164E+00 -4.032E-02 +-NEGLIGIBLE 2.212E+00 -1.048E-01 +-NEGLIGIBLE 2.255E+00 -1.290E-01 +-NEGLIGIBLE 2.291E+00 -1.613E-01 +-NEGLIGIBLE 2.327E+00 -1.855E-01 +-NEGLIGIBLE 2.370E+00 -1.774E-01 +-NEGLIGIBLE 2.412E+00 -1.774E-01 +-NEGLIGIBLE \END; /*===================================================================*/ |