/*===================================================================*/ /* NRDF D1581 Data No.9 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,9; 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,9; /* 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=74.72MEV; DELTA-INC-ENGY-LAB=0.1%; ANL=CC; /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,9; INC-ENGY-LAB=74.72MEV; DELTA-INC-ENGY-LAB=0.1%; SYS-ERR=X%'34'; /* '34' 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 (5.5%) */ 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) 3.254E-01 2.100E+00 +-NEGLIGIBLE 4.095E-01 2.558E+00 +-NEGLIGIBLE 4.937E-01 3.647E+00 +-NEGLIGIBLE 5.832E-01 5.200E+00 +-NEGLIGIBLE 6.619E-01 5.517E+00 +-NEGLIGIBLE 7.460E-01 6.588E+00 +-NEGLIGIBLE 8.299E-01 6.459E+00 +-NEGLIGIBLE 9.084E-01 5.739E+00 +-NEGLIGIBLE 9.871E-01 5.627E+00 +-NEGLIGIBLE 1.066E+00 4.712E+00 +-NEGLIGIBLE 1.144E+00 4.025E+00 +-NEGLIGIBLE 1.222E+00 3.177E+00 +-NEGLIGIBLE 1.301E+00 2.459E+00 +-NEGLIGIBLE 1.374E+00 1.794E+00 +-NEGLIGIBLE 1.452E+00 1.309E+00 +-NEGLIGIBLE 1.525E+00 1.033E+00 +-NEGLIGIBLE 1.604E+00 8.156E-01 +-NEGLIGIBLE 1.667E+00 6.831E-01 +-NEGLIGIBLE 1.740E+00 5.721E-01 +-NEGLIGIBLE 1.808E+00 4.697E-01 +-NEGLIGIBLE 1.871E+00 4.012E-01 +-NEGLIGIBLE 1.928E+00 3.636E-01 +-5.378E-02 1.996E+00 2.652E-01 +-NEGLIGIBLE 2.059E+00 2.178E-01 +-NEGLIGIBLE 2.116E+00 1.686E-01 +-NEGLIGIBLE 2.179E+00 1.254E-01 +-NEGLIGIBLE 2.231E+00 9.151E-02 +-NEGLIGIBLE 2.288E+00 6.418E-02 +-NEGLIGIBLE 2.346E+00 4.968E-02 +-NEGLIGIBLE 2.403E+00 3.349E-02 +-NEGLIGIBLE 2.450E+00 2.444E-02 +-NEGLIGIBLE 2.502E+00 1.748E-02 +-NEGLIGIBLE 2.554E+00 1.250E-02 +-NEGLIGIBLE 2.596E+00 1.089E-02 +-NEGLIGIBLE 2.643E+00 7.640E-03 +-NEGLIGIBLE 2.685E+00 7.947E-03 +-NEGLIGIBLE 2.727E+00 6.923E-03 +-NEGLIGIBLE 2.779E+00 5.574E-03 +-NEGLIGIBLE \END; /*===================================================================*/ |