/*===================================================================*/
 /* NRDF D1725 Data No.4                                              */
 /*===================================================================*/
 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,4;
 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,4;
 /* 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=208PB(6LI,6LI)X;
 PHQ=ANGL-DSTRN;
 THK-TGT=12.99MG/CM**2;
 DET-PARTCL=6LI;
 ANL=X'19';
 /* '19' CDCC (Coupled Discretized Continuum Channels) [Y.Sakuragi
         et al., Prog.Theor.Phys.98(1997)521] and single channel
         calculation */
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,4;
 INC-ENGY-LAB=100MEV/A;
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 THTC RUTH-RATIO DELTA-RUTH-RATIO
 (DEG) (NODIM) (NODIM)
 3.140E+00 5.237E-01 +-NEGLIGIBLE
 3.505E+00 3.249E-01 +-NEGLIGIBLE
 3.828E+00 2.742E-01 +-NEGLIGIBLE
 4.215E+00 2.659E-01 +-NEGLIGIBLE
 4.538E+00 1.895E-01 +-NEGLIGIBLE
 4.903E+00 1.072E-01 +-NEGLIGIBLE
 5.247E+00 9.330E-02 +-NEGLIGIBLE
 5.613E+00 1.039E-01 +-NEGLIGIBLE
 5.957E+00 7.999E-02 +-NEGLIGIBLE
 6.301E+00 4.000E-02 +-NEGLIGIBLE
 6.645E+00 2.639E-02 +-NEGLIGIBLE
 7.011E+00 3.761E-02 +-NEGLIGIBLE
 7.355E+00 3.274E-02 +-NEGLIGIBLE
 7.699E+00 1.662E-02 +-NEGLIGIBLE
 8.043E+00 6.398E-03 +-NEGLIGIBLE
 8.409E+00 1.016E-02 +-NEGLIGIBLE
 8.753E+00 1.563E-02 +-NEGLIGIBLE
 9.118E+00 1.114E-02 +-NEGLIGIBLE
 9.462E+00 3.908E-03 +-NEGLIGIBLE
 9.806E+00 2.387E-03 +-NEGLIGIBLE
 1.015E+01 5.401E-03 +-NEGLIGIBLE
 1.049E+01 6.015E-03 +-NEGLIGIBLE
 1.086E+01 3.299E-03 +-4.270E-04
 1.120E+01 1.289E-03 +-NEGLIGIBLE
 1.157E+01 1.527E-03 +-NEGLIGIBLE
 1.191E+01 2.500E-03 +-NEGLIGIBLE
 1.228E+01 2.078E-03 +-NEGLIGIBLE
 1.262E+01 1.008E-03 +-1.701E-04
 1.297E+01 5.788E-04 +-NEGLIGIBLE
 1.331E+01 8.123E-04 +-NEGLIGIBLE
 1.368E+01 9.475E-04 +-NEGLIGIBLE
 1.402E+01 7.181E-04 +-NEGLIGIBLE
 1.437E+01 2.806E-04 +-5.444E-05
 1.471E+01 1.969E-04 +-4.301E-05
 1.508E+01 2.894E-04 +-5.614E-05
 1.542E+01 3.536E-04 +-6.858E-05
 \END;
 /*===================================================================*/