/*===================================================================*/ /* NRDF D1840 Data No.2 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,2; D#=D1840; TITLE=/Pion-deuteron elastic scattering at large angles for momenta from 460 to 1160 MeV/c/; PURPOSE=/The differential cross section for pi- - d elastic scattering at c.m. pion angles 91 deg., 104 deg., 123 deg., 136 deg., and 155 deg. has been measured for pion momenta between 460 and 1160 MeV/c with the finest momentum steps so far employed./; ATH=(M.AKEMOTO'1', K.BABA'1', I.ENDO'1', H.HIMEMIYA'1', K.INOUE'1', T.KAWAMOTO'1', Y.MAEDA'1', T.OHSUGI'1', R.OHTANI'1', Y.SUMI'1', T.TAKESHITA'1', S.UEHARA'1', T.UMEDA'1', T.MAKI'2', M.NAKANO'2'); INST-ATH=(2JPNHIR'1', 2JPNKIT'2'); /* '1' Department of Physics */ REF=PRL; VLP=51(1983)1838; RCTS=D(PIN,PIN)D; PHQS=ANGL-DSTRN; /*===================================================================*/ /* Experimental Conditions */ /*===================================================================*/ \\EXP,2; /* 2003-11-11 : Compiled */ RTY=ELA-SCATT; PHQ=ANGL-DSTRN; CHM=ELM; PHYS-FORM=LIQD; THK-TGT=XMG/CM**2'3'; /* '3' 20 cm long and 5.5 cm in diameter */ POL-TGT=0%; ALGN-TGT=0%; ACC=SYN'4'; /* '4' pi-2 beam line */ INST-ACC=2JPNKEK; ERS-PRJ=2%; POL-PRJ=0%; DET-PARTCL=(PIN,D); COINC=(PIN,D); ANT-COINC=NO; DET-SYS=(MAG'5',MWPC'6',SCT'7',CRNKOV'8',TOF'9'); /* '5' Used to detect the recoil deuterons. The momentum resolution of the forward arm of the spectrometer which consisted of an analyzer magnet, five sets of MWPC's, and three sets of SC's was +-2.5 %. */ /* '6' Five sets of MWPC's (forward arm) are used to detect the recoil deuteron and two sets of MWPC's (backward arm) are used to detect the scattered pions. */ /* '7' Three sets of SC's (forward arm) are used to detect the recoil deuteron and two sets of SC's (backward arm) are used to detect the scattered pions. */ /* '8' Used to reject electron contamination in the incident beam /* '9' The particle identification for forward particles */ ANL=(GLAUBER'10',PSHIFT-ANL'11'); /* '10' [Ref. K. Kanai et al., Prog. Theor. Phys. 62, 153(1979), and 65, 266(1981).] */ /* '11' [Ref. N. Hiroshige et al., Prog. Theor. Phys. 68, 327(1982).] */ /* Experimental Method: - Time-of-flight (The particle identification for forward particles) /* Related references - R.C.Minehart, PRL, 46(1981)1185 - none, none, J(Sovi)31 RCT=D(PIN,PIN)D; INC-MOM-LAB=500[1160MEV/C; /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,2; SYS-ERR=(8%'17',<10%'18'); /* '17' An overall normalization uncertainty was estimated to be 8% */ /* '18' Maximum of systematic value is +-10%. Typical value is +-7%. (Not mentioned in the reference, but given in private communication.) */ RSD=D; THTC=104DEG'19'; /* '19' polar angle between deuteron and negative pion in the center of mass system */ DELTA-THTC=7'20'; /* '20' The bin width of theta was taken to be +-6 deg. to +-7 deg. */ /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; INC-MOM-LAB DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA'21' (GEV/C) (UB/SR) (UB/SR) 0.50 7.73 +-0.84 0.52 8.41 +-0.78 0.54 7.72 +-0.72 0.56 7.07 +-0.72 0.58 8.33 +-0.83 0.60 8.62 +-0.76 0.62 8.52 +-0.78 0.64 8.54 +-0.75 0.66 8.85 +-0.72 0.68 9.74 +-0.70 0.70 11.18 +-0.79 0.72 9.10 +-0.76 0.74 10.48 +-0.74 0.76 10.25 +-0.66 0.78 10.17 +-0.68 0.80 9.93 +-0.64 0.84 10.61 +-0.65 0.88 11.63 +-0.74 0.92 11.26 +-0.72 0.96 10.38 +-0.82 1.00 8.49 +-0.68 1.04 7.75 +-0.73 1.08 6.43 +-0.54 1.12 4.77 +-0.55 1.16 4.28 +-0.44 \END; /*===================================================================*/ |