/*===================================================================*/ /* NRDF D1581 Data No.10 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,10; 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,10; /* 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=54.70MEV; DELTA-INC-ENGY-LAB=0.1%; ANL=CC; /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,10; INC-ENGY-LAB=54.70MEV; DELTA-INC-ENGY-LAB=0.1%; SYS-ERR=5%'35'; /* '35' 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) 2.816E-01 2.457E-01 +-1.314E-01 3.592E-01 -1.314E-01 +-1.143E-01 4.272E-01 -7.429E-02 +-1.143E-01 4.272E-01 -1.714E-01 +-9.143E-02 4.951E-01 -1.029E-01 +-6.286E-02 5.631E-01 -1.086E-01 +-6.857E-02 6.359E-01 -5.714E-02 +-3.000E-02 7.039E-01 -6.857E-02 +-NEGLIGIBLE 7.718E-01 -6.857E-02 +-NEGLIGIBLE 8.495E-01 -6.857E-02 +-NEGLIGIBLE 9.126E-01 -6.857E-02 +-NEGLIGIBLE 9.757E-01 -1.657E-01 +-NEGLIGIBLE 9.757E-01 -6.286E-02 +-7.429E-02 1.044E+00 -1.200E-01 +-NEGLIGIBLE 1.102E+00 -1.143E-01 +-NEGLIGIBLE 1.170E+00 -1.143E-01 +-NEGLIGIBLE 1.233E+00 -1.371E-01 +-NEGLIGIBLE 1.296E+00 -1.429E-01 +-NEGLIGIBLE 1.359E+00 -1.943E-01 +-NEGLIGIBLE 1.417E+00 -1.600E-01 +-2.857E-02 1.476E+00 -1.257E-01 +-NEGLIGIBLE 1.539E+00 -7.429E-02 +-NEGLIGIBLE 1.592E+00 -4.000E-02 +-NEGLIGIBLE 1.646E+00 2.286E-02 +-NEGLIGIBLE 1.699E+00 9.714E-02 +-NEGLIGIBLE 1.752E+00 1.543E-01 +-4.000E-02 1.816E+00 1.943E-01 +-NEGLIGIBLE 1.874E+00 2.229E-01 +-NEGLIGIBLE 1.913E+00 2.229E-01 +-NEGLIGIBLE 1.961E+00 2.686E-01 +-NEGLIGIBLE 2.005E+00 2.286E-01 +-NEGLIGIBLE 2.053E+00 2.629E-01 +-NEGLIGIBLE 2.097E+00 2.514E-01 +-6.857E-02 2.136E+00 2.514E-01 +-NEGLIGIBLE 2.180E+00 2.057E-01 +-NEGLIGIBLE 2.228E+00 2.343E-01 +-NEGLIGIBLE 2.267E+00 2.571E-01 +-NEGLIGIBLE 2.306E+00 2.457E-01 +-3.429E-02 2.350E+00 3.143E-01 +-NEGLIGIBLE 2.383E+00 3.143E-01 +-NEGLIGIBLE \END; /*===================================================================*/ |