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 /* NRDF D0883 Data No.21                                             */
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 /* Bibliography                                                      */
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 \\BIB,21;
 D#=D883;
 TITLE=/ Deuteron breakup with 3He at 89.4 and 118.9 MeV /;
 ATH=(K.FUKUNAGA'1', S.KAKIGI'1', T.OHSAWA'1', A.OKIHANA'2',
      S.TANAKA'3', T.SEKIOKA'4', H.NAKAMURA-YOKOTA'5', S.KATO'6');
 INST-ATH=(2JPNKTO'1', 2JPNKUE'2', 2JPNJPN'3', 2JPNHIT'4', 2JPNTIT'5',
           2JPNYMG'6');
      /* '1' Institute for Chemical Resarch */
      /* '3' Hosoda Jutaku, 1-12-10, Santanda, Amagasaki */
      /* '5' Faculty of Science */
      /* '6' Faculty of General Education */
 REF=NP/A;
 VLP=369(1981)289;
 RCTS=(2H(3HE,P,3HE)N, 2H(3HE,2*P)T, 2H(3HE,P,T)P, 2H(3HE,D,D)P);
 PHQS=TRPL-DIFF-XSECTN;
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 /* Experimental Conditions                                           */
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 \\EXP,21;
 /* 2005-08-18 : Altered, At. Re-digitized */
 /* 2005-07-23 : Converted, Am + On. Converted to EXFOR E0883 */
 PHQ=TRPL-DIFF-XSECTN;
 CHM=ELM;
 PHYS-FORM=GAS;
 THK-TGT=XMG/CM**2'7';
 /* '7' 2.95 atm */
 BAC=X'8';
 /* '8' Gass cell with windows of 10 micro-meter Havar foil used */
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=CYC'9';
 /* '9' Isochronous cyclotron */
 INST-ACC=2JPNRCN;
 BEAM-INTNSTY=<150NA'10';
 /* '10' Several tens of nA to 150 nA */
 CHRG-INC-ION=2+;
 POL-PRJ=0%;
 ANT-COINC=NO;
 DET-SYS=(SI'11',NAI'12',EDE);
 /* '11' Used as E and Delta-E detector */
 /* '12' Used as E detector */
 ANL=X'13';
 /* '13' Three- and four-body spectator model */
 /* Experimental Method:
    - Particle identification by 'E/Delta E' measurement
 RCT=2H(3HE,D,D)P;
 INC-ENGY-LAB=89.4MEV;
 DET-PARTCL=(D,D);
 COINC=(D,D);
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 /* Descriptive Parameters                                            */
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 \\DATA,21;
 INC-ENGY-LAB=89.4MEV;
 EMT-1=D;
 EMT-2=D;
 THTL-1=30DEG;
 THTL-2=20DEG;
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 /* Data Table                                                        */
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 \DATA;
 ENGY-EMT'16' DSIGMA/DOMEGA/DOMEGA/DE
 DELTA-DSIGMA/DOMEGA/DOMEGA/DE
 (MEV) (MB/SR**2/MEV) (MB/SR**2/MEV)
 8.796E+00 1.122E-01 +-1.425E-01
 9.907E+00 2.684E-01 +-1.852E-01
 1.139E+01 2.535E-01 +-1.567E-01
 1.278E+01 6.803E-01 +-1.424E-01
 1.389E+01 5.088E-01 +-1.852E-01
 1.546E+01 9.782E-01 +-1.709E-01
 1.657E+01 8.638E-01 +-1.710E-01
 1.806E+01 1.860E+00 +-2.280E-01
 1.944E+01 2.031E+00 +-2.280E-01
 2.065E+01 2.871E+00 +-2.707E-01
 2.167E+01 4.466E+00 +-2.991E-01
 2.324E+01 5.576E+00 +-3.846E-01
 2.444E+01 7.014E+00 +-4.701E-01
 2.574E+01 8.025E+00 +-4.416E-01
 2.694E+01 8.637E+00 +-5.413E-01
 2.824E+01 8.451E+00 +-5.841E-01
 2.935E+01 8.337E+00 +-4.558E-01
 3.083E+01 6.456E+00 +-3.277E-01
 3.241E+01 5.686E+00 +-4.132E-01
 3.324E+01 4.190E+00 +-3.420E-01
 3.481E+01 3.377E+00 +-3.562E-01
 3.593E+01 2.479E+00 +-3.134E-01
 3.731E+01 2.479E+00 +-2.992E-01
 3.880E+01 1.566E+00 +-1.995E-01
 3.991E+01 1.637E+00 +-2.137E-01
 4.139E+01 1.223E+00 +-1.995E-01
 4.241E+01 7.527E-01 +-1.710E-01
 4.389E+01 6.239E-01 +-1.709E-01
 4.500E+01 7.943E-01 +-1.994E-01
 4.676E+01 -3.263E-02 +-1.282E-01
 4.796E+01 1.093E-01 +-9.975E-02
 4.935E+01 3.651E-01 +-1.282E-01
 5.046E+01 4.643E-01 +-1.567E-01
 5.176E+01 5.920E-01 +-1.852E-01
 5.287E+01 5.487E-01 +-1.852E-01
 \END;
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