/*===================================================================*/
 /* NRDF D1725 Data No.2                                              */
 /*===================================================================*/
 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,2;
 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,2;
 /* 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=58NI(6LI,6LI)X;
 PHQ=ANGL-DSTRN;
 THK-TGT=(4.00MG/CM**2,5.86MG/CM**2);
 DET-PARTCL=6LI;
 ANL=X'17';
 /* '17' CDCC (Coupled Discretized Continuum Channels) [Y.Sakuragi
         et al., Prog.Theor.Phys.98(1997)521] and single channel
         calculation */
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,2;
 INC-ENGY-LAB=100MEV/A;
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 THTC RUTH-RATIO DELTA-RUTH-RATIO
 (DEG) (NODIM) (NODIM)
 2.848E+00 9.035E-02 +-9.312E-03
 3.237E+00 1.735E-01 +-1.957E-02
 3.627E+00 2.957E-01 +-3.335E-02
 4.039E+00 2.624E-01 +-2.704E-02
 4.406E+00 1.135E-01 +-1.443E-02
 4.795E+00 2.821E-02 +-3.586E-03
 5.208E+00 5.847E-02 +-5.316E-03
 5.574E+00 1.411E-01 +-1.455E-02
 5.964E+00 1.812E-01 +-2.044E-02
 6.354E+00 1.442E-01 +-1.833E-02
 6.743E+00 7.348E-02 +-8.444E-03
 7.110E+00 3.584E-02 +-4.386E-03
 7.499E+00 4.407E-02 +-4.542E-03
 7.912E+00 7.509E-02 +-8.469E-03
 8.278E+00 8.744E-02 +-1.005E-02
 8.668E+00 7.758E-02 +-8.916E-03
 9.034E+00 5.598E-02 +-6.433E-03
 9.447E+00 3.431E-02 +-3.537E-03
 9.836E+00 2.672E-02 +-2.754E-03
 1.023E+01 2.760E-02 +-2.574E-03
 1.062E+01 3.180E-02 +-3.277E-03
 1.098E+01 3.145E-02 +-3.614E-03
 1.137E+01 2.422E-02 +-2.784E-03
 1.176E+01 1.806E-02 +-2.037E-03
 1.217E+01 1.026E-02 +-1.179E-03
 1.256E+01 7.647E-03 +-1.008E-03
 1.293E+01 8.342E-03 +-1.100E-03
 1.332E+01 7.564E-03 +-9.975E-04
 1.371E+01 7.900E-03 +-9.668E-04
 1.410E+01 5.639E-03 +-7.436E-04
 1.449E+01 4.113E-03 +-5.810E-04
 1.488E+01 3.419E-03 +-5.147E-04
 1.524E+01 2.936E-03 +-4.420E-04
 1.566E+01 2.165E-03 +-4.042E-04
 1.605E+01 1.942E-03 +-3.966E-04
 1.641E+01 1.512E-03 +-3.347E-04
 1.680E+01 1.103E-03 +-2.982E-04
 \END;
 /*===================================================================*/