/*===================================================================*/ /* NRDF D1733 Data No.8 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,8; D#=D1733; TITLE=/ Double-pion production induced by deutron-proton collisions in the incident deutron momentum range 2.1-3.8 GeV/c /; PURPOSE=/ The purpose of this experiment is (1) to extend the analysis of d-p interactions to obtain the d-p double-pion production cross sections, and from them deduce the p-p and n-p double-pion production cross sections, (2) to analyze the N-N double-pion production data in terms of various production mechanisms such as N-N double-pion production with one nucleon in the deuteron and the other as the spectator nucleon, and two sequential N-N single-pion production reactions involving all two nucleons in the deuteron, and (3) to analyze the d-p double-pion production reactions as the sum of the N-N double-pion production reactions and two sequential N-N single-pion production reactions. /; ATH=(T.TSUBOYAMA'1', F.SAI'1', N.KATAYAMA'1', T.KISHIDA'1', S.S.YAMAMOTO'1'); INST-ATH=(2JPNTOK'1'); /* '1' Department of Physics */ REF=PR/C; VLP=62(2000)034001; RCTS=(P(D,PIN,PIP,N,P)P, P(D,PIN,PI0,P,P)P, P(D,PIN,PIP,P)D, P(D,PIN,PIP,D)P); PHQS=(TOT-XSECTN, MOM-DSTRN'2', MOM-DSTRN'3', MOM-DSTRN'4', ENGY-SPEC'5'); /* '2' Momentum distributions of the slowest proton in the deuteron rest frame */ /* '3' Momentum distributions of the slowest neutron in the deuteron rest frame */ /* '4' Momentum distributions of proton in the deuteron rest frame /* '5' Invariant mass distribution among N-pi-pi */ /*===================================================================*/ /* Experimental Conditions */ /*===================================================================*/ \\EXP,8; /* 2002-02-03 : Compiled */ CHM=ELM; PHYS-FORM=LIQD'6'; /* '6' KEK 1m bubble chamber filled with liquid hydrogen */ BAC=X; POL-TGT=0%; ALGN-TGT=0%; ACC=SYN; INST-ACC=2JPNKEK; ERS-PRJ=1%'7'; /* '7' See [N.Katayama et al., NP/A438(1985)685] */ POL-PRJ=0%; COINC=NO; ANT-COINC=NO; DET-SYS=(BUBBLC,TOF'8'); /* '8' See [N.Katayama et al., NP/A438(1985)685] */ /* Experimental Method: - Time-of-flight (See [N.Katayama et al., NP/A438(1985)685]) /* 2006-08-24 : Altered, At. Re-digitized */ RCT=(P(D,PIN,PIP,N,P)P+P(D,PIN,PI0,P,P)P+P(D,PIN,PIP,D)P); PHQ=ENGY-SPEC'25'; /* '25' Invariant mass distribution among N-pi-pi */ INC-MOM-LAB=3.79GEV/C; DET-PARTCL=(PIP,PIN,D,P); /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,8; INC-MOM-LAB=3.79GEV/C; /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; DATA1'26' DATA2'27' DELTA-DATA2'27,28' (UNIT1) (UNIT2) (UNIT1) 1.209E+00 1.993E+00 +-NEGLIGIBLE 1.230E+00 4.376E+00 +-NEGLIGIBLE 1.269E+00 1.514E+01 +-3.998E+00 1.290E+00 3.593E+01 +-6.400E+00 1.311E+00 6.471E+01 +-8.000E+00 1.331E+00 7.790E+01 +-8.800E+00 1.351E+00 1.107E+02 +-1.000E+01 1.371E+00 1.391E+02 +-1.120E+01 1.392E+00 1.598E+02 +-1.200E+01 1.411E+00 1.466E+02 +-1.200E+01 1.431E+00 1.290E+02 +-1.120E+01 1.451E+00 1.102E+02 +-1.040E+01 1.471E+00 8.378E+01 +-8.799E+00 1.491E+00 4.977E+01 +-6.799E+00 1.511E+00 4.415E+01 +-6.399E+00 1.531E+00 2.814E+01 +-5.200E+00 1.551E+00 1.492E+01 +-3.600E+00 1.570E+00 8.104E+00 +-2.801E+00 1.590E+00 6.888E+00 +-2.800E+00 1.609E+00 2.074E+00 +-NEGLIGIBLE \END; /*===================================================================*/ |