/*===================================================================*/
 /* NRDF D1733 Data No.5                                              */
 /*===================================================================*/
 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,5;
 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,5;
 /* 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;
 PHQ=MOM-DSTRN'13';
 /* '13' Momentum distributions of the slowest neutron in the
         deuteron rest frame */
 INC-MOM-LAB=3.79GEV/C;
 DET-PARTCL=(PIP,PIN,P);
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,5;
 INC-MOM-LAB=3.79GEV/C;
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 MOM-EMT'14' DATA1'15' DELTA-DATA1'15,16'
 (GEV) (NODIM) (NODIM)
 3.558E-02 6.003E+00 +-2.450E+00
 4.417E-02 5.008E+00 +-2.236E+00
 5.399E-02 4.012E+00 +-2.006E+00
 6.503E-02 2.006E+00 +-1.409E+00
 7.485E-02 3.997E+00 +-2.006E+00
 8.466E-02 4.992E+00 +-2.236E+00
 9.448E-02 1.011E+00 +-9.954E-01
 1.055E-01 3.997E+00 +-2.006E+00
 1.153E-01 2.006E+00 +-1.409E+00
 1.252E-01 1.011E+00 +-9.954E-01
 1.362E-01 1.011E+00 +-9.954E-01
 1.448E-01 3.002E+00 +-1.730E+00
 1.534E-01 1.991E+00 +-1.409E+00
 1.656E-01 1.011E+00 +-9.951E-01
 1.755E-01 2.006E+00 +-1.394E+00
 1.951E-01 1.011E+00 +-9.954E-01
 2.135E-01 1.011E+00 +-9.954E-01
 2.245E-01 1.011E+00 +-9.954E-01
 2.356E-01 1.991E+00 +-1.409E+00
 2.454E-01 1.991E+00 +-1.409E+00
 2.564E-01 1.991E+00 +-1.409E+00
 2.650E-01 1.011E+00 +-9.951E-01
 2.748E-01 1.991E+00 +-1.409E+00
 2.957E-01 1.011E+00 +-9.954E-01
 3.153E-01 1.011E+00 +-9.954E-01
 3.448E-01 3.002E+00 +-1.730E+00
 3.558E-01 1.011E+00 +-9.954E-01
 3.669E-01 1.011E+00 +-9.954E-01
 3.742E-01 1.011E+00 +-9.954E-01
 3.951E-01 2.006E+00 +-1.409E+00
 4.061E-01 1.011E+00 +-9.954E-01
 4.147E-01 1.011E+00 +-9.954E-01
 4.442E-01 1.011E+00 +-9.954E-01
 4.748E-01 1.011E+00 +-9.954E-01
 4.859E-01 1.011E+00 +-9.954E-01
 5.362E-01 1.011E+00 +-9.954E-01
 5.755E-01 1.011E+00 +-9.954E-01
 5.951E-01 1.991E+00 +-1.409E+00
 6.454E-01 1.011E+00 +-9.954E-01
 6.564E-01 1.011E+00 +-9.954E-01
 \END;
 /*===================================================================*/