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| /*===================================================================*/
/* 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;
/*===================================================================*/
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