/*===================================================================*/
 /* NRDF D1594 Data No.3                                              */
 /*===================================================================*/
 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,3;
 D#=D1594;
 TITLE=/ Elastic scattering of 3He particles at 450 MeV /;
 PURPOSE=/ To measure elastic scattering of 3He particles at an
           incident energy of 150 MeV/nucleon for several target nuclei
           in a wide mass region. /;
 ATH=(T.YAMAGATA'1', H.UTSUNOMIYA'1', M.TANAKA'2', S.NAKAYAMA'3',
      N.KOORI'3', A.TAMII'4', Y.FUJITA'5', K.KATORI'5', M.INOUE'6',
      M.FUJIWARA'7', H.OGATA'7');
 INST-ATH=(2JPNKON'1', 2JPNKTJ'2', 2JPNTKS'3', 2JPNKTO'4', 2JPNOSA'5',
           2JPNKTO'6', 2JPNRCN'7');
      /* '1' Department of Physics */
      /* '3' Department of Physics */
      /* '4' Department of Physics */
      /* '5' Department of Physics */
      /* '6' Institute for Chemical Research */
 REF=(NP/A'8');
 VLP=(589(1995)425'8');
 /* Secondary reference 
    - PR/C, 50(1994)2606 (Brief report for 90Zr and 208Pb target)
 RCTS=(12C(3HE,3HE)12C, 28SI(3HE,3HE)28SI, 58NI(3HE,3HE)58NI,
       90ZR(3HE,3HE)90ZR, 208PB(3HE,3HE)208PB);
 PHQS=(ANGL-DSTRN, OPT-POTL-PARA);
 /*===================================================================*/
 /* Experimental Conditions                                           */
 /*===================================================================*/
 \\EXP,3;
 /* 2005-09-09 : Converted, Sr + On. Converted to EXFOR E1594 */
 /* 2005-09-26 : Altered, At + Ot + Sr. Re-digitized */
 RTY=ELA-SCATT;
 CHM=ELM;
 PHYS-FORM=SLD;
 BAC=SELF;
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=CYC'9';
 /* '9' K = 400 MeV ring cyclotron */
 INST-ACC=2JPNRCN;
 INC-ENGY-LAB=450MEV;
 BEAM-INTNSTY=1[30NA;
 POL-PRJ=0%;
 DET-PARTCL=3HE;
 COINC=NO;
 ANT-COINC=NO;
 DET-SYS=(MAG'10',MWDC'11',SCT'12',TOF);
 /* '10' Grand RAIDEN: To analyze 3He [M.Fujiwara, et al., Nucl.
         Instr. Meth. A, to be published]. */
 /* '11' To detect 3He by two 2-dimensional position-sensitive
         multiwire-drift-chambers */
 /* '12' To detect 3He by two plastic scintillators (delta E)
         [T.Noro, et al., RCNP annual report (1991) p.177,
         unpublished.] */
 ERS-DET=400KEV'13';
 /* '13' Mainly due to energy spread of incident beam */
 ANL=OPT-MODEL'14';
 /* '14' Analysis using the code 'ECIS' [Ref: J. Raynal, Code
         ECIS88, unpublished.] */
 /* Experimental Method:
    - Time-of-flight
 RCT=58NI(3HE,3HE)58NI;
 PHQ=ANGL-DSTRN;
 ENR=>99%'22';
 /* '22' Larger than 99% for thick target while unknown for thin
         target */
 THK-TGT=(52.0MG/CM**2, 5.9MG/CM**2)'23';
 /* '23' Thin target (5.9 mg/cm**2) was used for measurement at
         forward-scattering angle */
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,3;
 INC-ENGY-LAB=450MEV;
 SYS-ERR=15%'24';
 /* '24' Total systematic error. Uncertainty in absolute value,
         mainly due to the uncertainty in target thickness and the
         charge-collection efficiency of Faraday cup */
 EMT=3HE;
 DELTA-THTL=0.05DEG;
 DATA1=0.3DEG'25';
 /* '25' Overall angular resolution */
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 THTC RUTH-RATIO DELTA-RUTH-RATIO'26'
 (DEG) (NODIM) (NODIM)
 3.854E+00 1.879E-01 +-NEGLIGIBLE
 4.355E+00 4.256E-02 +-NEGLIGIBLE
 4.857E+00 2.877E-02 +-NEGLIGIBLE
 5.358E+00 1.603E-01 +-NEGLIGIBLE
 6.003E+00 3.780E-01 +-NEGLIGIBLE
 6.433E+00 4.416E-01 +-NEGLIGIBLE
 7.006E+00 3.773E-01 +-NEGLIGIBLE
 7.507E+00 2.359E-01 +-NEGLIGIBLE
 8.009E+00 1.594E-01 +-NEGLIGIBLE
 8.582E+00 5.998E-02 +-NEGLIGIBLE
 9.155E+00 9.956E-02 +-NEGLIGIBLE
 9.656E+00 1.414E-01 +-NEGLIGIBLE
 1.023E+01 1.856E-01 +-NEGLIGIBLE
 1.073E+01 1.715E-01 +-NEGLIGIBLE
 1.123E+01 1.115E-01 +-NEGLIGIBLE
 1.181E+01 5.732E-02 +-NEGLIGIBLE
 1.223E+01 3.875E-02 +-NEGLIGIBLE
 1.288E+01 3.722E-02 +-NEGLIGIBLE
 1.338E+01 4.521E-02 +-NEGLIGIBLE
 1.388E+01 4.883E-02 +-NEGLIGIBLE
 1.453E+01 4.690E-02 +-NEGLIGIBLE
 1.496E+01 3.565E-02 +-NEGLIGIBLE
 1.553E+01 2.228E-02 +-NEGLIGIBLE
 1.610E+01 1.393E-02 +-NEGLIGIBLE
 1.660E+01 1.018E-02 +-NEGLIGIBLE
 1.711E+01 9.782E-03 +-NEGLIGIBLE
 1.761E+01 9.772E-03 +-NEGLIGIBLE
 1.818E+01 9.761E-03 +-NEGLIGIBLE
 1.868E+01 8.341E-03 +-NEGLIGIBLE
 1.926E+01 6.339E-03 +-NEGLIGIBLE
 1.990E+01 3.962E-03 +-NEGLIGIBLE
 2.040E+01 2.291E-03 +-NEGLIGIBLE
 2.090E+01 1.489E-03 +-NEGLIGIBLE
 2.133E+01 1.431E-03 +-NEGLIGIBLE
 2.198E+01 1.671E-03 +-NEGLIGIBLE
 2.248E+01 1.320E-03 +-NEGLIGIBLE
 2.298E+01 1.426E-03 +-NEGLIGIBLE
 2.351E+01 9.256E-04 +-NEGLIGIBLE
 2.405E+01 8.237E-04 +-NEGLIGIBLE
 2.463E+01 5.567E-04 +-4.524E-05
 2.513E+01 3.347E-04 +-2.720E-05
 2.575E+01 2.805E-04 +-1.992E-05
 2.617E+01 2.146E-04 +-2.907E-05
 2.678E+01 1.413E-04 +-3.047E-05
 2.728E+01 1.855E-04 +-2.307E-05
 2.785E+01 1.206E-04 +-3.185E-05
 2.835E+01 9.910E-05 +-1.232E-05
 2.885E+01 6.699E-05 +-1.445E-05
 2.936E+01 6.436E-05 +-1.388E-05
 \END;
 /*===================================================================*/