/*===================================================================*/
 /* NRDF D1725 Data No.3                                              */
 /*===================================================================*/
 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,3;
 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,3;
 /* 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=90ZR(6LI,6LI)X;
 PHQ=ANGL-DSTRN;
 THK-TGT=7.34MG/CM**2;
 DET-PARTCL=6LI;
 ANL=X'18';
 /* '18' CDCC (Coupled Discretized Continuum Channels) [Y.Sakuragi
         et al., Prog.Theor.Phys.98(1997)521] and single channel
         calculation */
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,3;
 INC-ENGY-LAB=100MEV/A;
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 THTC RUTH-RATIO DELTA-RUTH-RATIO
 (DEG) (NODIM) (NODIM)
 2.526E+00 1.843E-01 +-1.886E-02
 2.892E+00 3.239E-01 +-3.661E-02
 3.235E+00 3.696E-01 +-3.781E-02
 3.601E+00 2.315E-01 +-NEGLIGIBLE
 3.990E+00 7.681E-02 +-NEGLIGIBLE
 4.356E+00 3.278E-02 +-3.736E-03
 4.722E+00 7.148E-02 +-7.313E-03
 5.088E+00 1.212E-01 +-1.240E-02
 5.454E+00 1.101E-01 +-1.244E-02
 5.820E+00 4.928E-02 +-4.963E-03
 6.209E+00 1.302E-02 +-NEGLIGIBLE
 6.552E+00 2.548E-02 +-2.880E-03
 6.941E+00 5.760E-02 +-6.510E-03
 7.284E+00 6.264E-02 +-7.982E-03
 7.650E+00 4.068E-02 +-NEGLIGIBLE
 8.016E+00 1.957E-02 +-2.231E-03
 8.382E+00 1.256E-02 +-1.285E-03
 8.771E+00 2.129E-02 +-2.631E-03
 9.114E+00 2.873E-02 +-3.247E-03
 9.480E+00 2.738E-02 +-3.489E-03
 9.846E+00 1.866E-02 +-2.108E-03
 1.021E+01 1.037E-02 +-1.172E-03
 1.058E+01 8.556E-03 +-8.754E-04
 1.094E+01 1.049E-02 +-1.186E-03
 1.131E+01 1.183E-02 +-1.337E-03
 1.168E+01 1.037E-02 +-1.321E-03
 1.204E+01 6.978E-03 +-8.891E-04
 1.241E+01 5.048E-03 +-6.432E-04
 1.277E+01 3.565E-03 +-4.779E-04
 1.314E+01 3.398E-03 +-4.906E-04
 1.351E+01 3.972E-03 +-5.323E-04
 1.387E+01 3.481E-03 +-4.908E-04
 1.426E+01 2.400E-03 +-3.709E-04
 1.460E+01 1.675E-03 +-2.924E-04
 1.499E+01 1.114E-03 +-2.055E-04
 1.534E+01 1.382E-03 +-2.550E-04
 1.570E+01 1.062E-03 +-2.164E-04
 1.607E+01 1.127E-03 +-2.189E-04
 \END;
 /*===================================================================*/