/*===================================================================*/
 /* NRDF D1725 Data No.1                                              */
 /*===================================================================*/
 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,1;
 D#=D1725;
 TITLE=/ Reaction mechanism of 6Li scattering at 600 MeV /;
 PURPOSE=/ To study the role of the breakup channels and its feedback
           to the elastic scattering at intermediate energy /;
 ATH=(K.SCHWARZ'1,2', C.SAMANTA'1,3', M.FUJIWARA'1,6', H.REBEL'2',
      R.DE.LEO'4', N.MATSUOKA'1', H.UTSUNOMIYA'5', H.AKIMUNE'6',
      I.DAITO'1', H.FUJIMURA'1', F.IHARA'1', K.ISHIBASHI'1', Y.MAEDA'1',
      T.YAMANAKA'1', H.YOSHIDA'1', A.OKIHANA'7', T.YOSHIMURA'7',
      P.K.J.VAN AARLE'1,8', W.A.T.UIJEN'1,8', M.ITO'9', Y.SAKURAGI'9');
 INST-ATH=(2JPNRCN'1', 2GERKFK'2', 3INDSAH'3', 2ITYBAU'4', 2JPNKON'5',
           2JPNJAE'6', 2JPNKUE'7', 2NEDENT'8', 2JPNJPN'9');
      /* '4' Dipartimento di Fisica */
      /* '6' Advanced Science Research Center */
      /* '9' Department of Physcics, Osaka City University, Osaka */
 REF=EPJ/A;
 VLP=7(2000)367;
 RCTS=(12C(6LI,6LI)X, 58NI(6LI,6LI)X, 90ZR(6LI,6LI)X, 208PB(6LI,6LI)X,
       12C(6LI,ALPHA)X, 58NI(6LI,ALPHA)X, 90ZR(6LI,ALPHA)X,
       208PB(6LI,ALPHA)X);
 PHQS=(ANGL-DSTRN, X'10', DATA'11', DATA'12');
 /* '10' Transverse momentum distribution */
 /* '11' Double differential cross section against logitudinal
    momentum of alpha. */
 /* '12' squared of absolute value of momentum distribution */
 /*===================================================================*/
 /* Experimental Conditions                                           */
 /*===================================================================*/
 \\EXP,1;
 /* 2002-09-27 : Converted, Ay + On. Data converted to EXFOR E1725
 ENR=X%;
 CHM=ELM;
 PHYS-FORM=SLD;
 BAC=SELF;
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=CYC'13';
 /* '13' Ring Cyclotron */
 INST-ACC=2JPNRCN;
 INC-ENGY-LAB=100MEV/A;
 BEAM-INTNSTY=1NA;
 POL-PRJ=0%;
 COINC=NO;
 ANT-COINC=NO;
 DET-SYS=(MAG'14',MWDC,SCT'15',EDE);
 /* '14' Grand Gaiden [M.Fujiwara et al., Nucl.Instr.and Meth.in
         Phys.Res.A422(1999)484] */
 /* '15' To measure energy loss Delta E and the residual energy E
         to particle identification */
 /* Experimental Method:
    - Particle identification by 'E/Delta E' measurement
 /* 2006-08-08 : Altered, At. Re-digitized */
 RCT=12C(6LI,6LI)X;
 PHQ=ANGL-DSTRN;
 THK-TGT=(4.1MG/CM**2,30MG/CM**2);
 DET-PARTCL=6LI;
 ANL=X'16';
 /* '16' CDCC (Coupled Discretized Continuum Channels) [Y.Sakuragi
         et al., Prog.Theor.Phys.98(1997)521] and single channel
         calculation */
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,1;
 INC-ENGY-LAB=100MEV/A;
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 THTC RUTH-RATIO DELTA-RUTH-RATIO
 (DEG) (NODIM) (NODIM)
 4.094E+00 3.521E+00 +-NEGLIGIBLE
 4.638E+00 2.717E+00 +-NEGLIGIBLE
 5.145E+00 1.775E+00 +-NEGLIGIBLE
 5.688E+00 1.559E+00 +-NEGLIGIBLE
 6.196E+00 2.216E+00 +-NEGLIGIBLE
 6.739E+00 3.456E+00 +-NEGLIGIBLE
 7.246E+00 4.647E+00 +-NEGLIGIBLE
 7.717E+00 5.193E+00 +-NEGLIGIBLE
 8.261E+00 4.396E+00 +-NEGLIGIBLE
 8.804E+00 2.618E+00 +-NEGLIGIBLE
 9.312E+00 1.742E+00 +-NEGLIGIBLE
 9.819E+00 1.203E+00 +-NEGLIGIBLE
 1.036E+01 1.077E+00 +-NEGLIGIBLE
 1.087E+01 1.057E+00 +-NEGLIGIBLE
 1.138E+01 1.117E+00 +-NEGLIGIBLE
 1.188E+01 1.138E+00 +-NEGLIGIBLE
 1.243E+01 9.286E-01 +-NEGLIGIBLE
 1.293E+01 8.785E-01 +-NEGLIGIBLE
 1.344E+01 6.779E-01 +-NEGLIGIBLE
 1.395E+01 5.429E-01 +-NEGLIGIBLE
 1.449E+01 3.355E-01 +-NEGLIGIBLE
 1.500E+01 2.589E-01 +-NEGLIGIBLE
 1.554E+01 1.998E-01 +-NEGLIGIBLE
 1.605E+01 1.723E-01 +-NEGLIGIBLE
 1.659E+01 1.330E-01 +-NEGLIGIBLE
 1.710E+01 1.190E-01 +-NEGLIGIBLE
 1.761E+01 9.708E-02 +-NEGLIGIBLE
 1.812E+01 7.220E-02 +-NEGLIGIBLE
 1.862E+01 7.087E-02 +-NEGLIGIBLE
 1.917E+01 4.895E-02 +-NEGLIGIBLE
 1.967E+01 3.708E-02 +-NEGLIGIBLE
 2.018E+01 2.969E-02 +-NEGLIGIBLE
 2.072E+01 2.334E-02 +-NEGLIGIBLE
 2.123E+01 1.525E-02 +-NEGLIGIBLE
 2.174E+01 1.267E-02 +-NEGLIGIBLE
 2.228E+01 9.780E-03 +-NEGLIGIBLE
 2.279E+01 8.128E-03 +-NEGLIGIBLE
 2.330E+01 5.023E-03 +-NEGLIGIBLE
 2.540E+01 3.405E-03 +-6.783E-04
 2.591E+01 2.105E-03 +-4.804E-04
 2.641E+01 1.954E-03 +-4.738E-04
 2.692E+01 1.849E-03 +-4.739E-04
 \END;
 /*===================================================================*/