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 /* NRDF D1827 Data No.2                                              */
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 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,2;
 D#=D1827;
 TITLE=/ Momentum distributions of 14C and 15C fragments from 16C
         breakup /;
 ATH=(T.YAMAGUCHI'1', T.ZHENG'1,2,3', A.OZAWA'1', M.CHIBA'1,4',
      R.KANUNGO'1', T.KATO'1', K.MORIMOTO'1', T.OHNISHI'1', T.SUDA'1',
      Y.YAMAGUCHI'1,5', A.YOSHIDA'1', K.YOSHIDA'1', I.TANIHATA'1');
 INST-ATH=(2JPNIPC'1', 2JPNSUT'2', 3CPRBJG'3', 2JPNTOH'4',
           2JPNNII'5');
      /* '2' Department of Physics */
      /* '3' Department of Technical Physics */
      /* '4' Department of Physics */
      /* '5' Department of Physics */
 REF=NP/A;
 VLP=724(2003)3;
 RCTS=(C(16C,15C)X, C(16C,14C)X);
 PHQS=(MOM-DSTRN'6', XSECTN'7', XSECTN'8');
 /* '6' longitudinal momentum distribution */
 /* '7' one neutron removal cross section */
 /* '8' two neutrons removal cross section */
 /*===================================================================*/
 /* Experimental Conditions                                           */
 /*===================================================================*/
 \\EXP,2;
 /* 2003-09-01 : Compiled, Km + Am */
 ENR=NAT;
 CHM=ELM;
 PHYS-FORM=SLD;
 THK-TGT=370MG/CM**2;
 BAC=X;
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=PRJFS'9';
 /* '9' Primary beam, 22Ne of 110 AMeV, was used to bombard a Be
        target to produce a 16C secondary beam through the projectile
        fragmentation reaction. */
 INST-ACC=2JPNIPC;
 INC-ENGY-LAB=83MEV/A'10';
 /* '10' Around 83 MeV/A at the middle of the carbon target. */
 ERS-PRJ=XKEV'11';
 /* '11' The momentum broadening was confined to +-0.4 percent by
         a momentum slit. */
 POL-PRJ=0%;
 COINC=NO;
 ANT-COINC=NO;
 DET-SYS=(MAG,SCT'12',NAI'13',SI'14',TOF'15',EDE'16');
 /* '12' To obtain ToF signal */
 /* '13' NaI(Tl) detector to measure total energy */
 /* '14' To identify charge of fragment */
 /* '15' To obtain fragment velocity */
 /* '16' To identify particles */
 CALB-DET=/ TOF was calibrated by using the primary beam with several
            energies obtained by passing through different thicknesses
            of Be (2, 4, 7.5, 9 mm). /;
 /* Experimental Method:
    - Time-of-flight (To obtain fragment velocity)
    - Particle identification by 'E/Delta E' measurement (To identify
      particles)
 /* 2006-11-21 : Altered, On. Data replaced by authors' tabulated
    data */
 RCT=C(16C,14C)X;
 RTY=INCL;
 PHQ=MOM-DSTRN'21';
 /* '21' longitudinal momentum distribution */
 DET-PARTCL=14C;
 ANL=GLAUBER;
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 /* Descriptive Parameters                                            */
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 \\DATA,2;
 INC-ENGY-LAB=83MEV/A'17';
 /* '17' Around 83 MeV/A at the middle of the carbon target. */
 WDTH=142MEV/C'22';
 /* '22' Width of momentum distribution obtained from the
         Lorentzian function fit to the distribution in the projectile
         rest frame */
 DELTA-WDTH=14MEV/C;
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 MOM-LNGTD'23' DSIGMA/DPL DELTA-DSIGMA/DPL
 (MEV/C) (MB/(MEV/C)) (MB/(MEV/C))
 -280 0.070 +-0.020
 -240 0.103 +-0.024
 -200 0.082 +-0.020
 -160 0.154 +-0.027
 -120 0.218 +-0.032
 -80 0.324 +-0.038
 -40 0.352 +-0.078
 0 0.773 +-0.151
 40 0.515 +-0.085
 80 0.305 +-0.034
 120 0.137 +-0.022
 160 0.073 +-0.016
 200 0.041 +-0.011
 \END;
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