/*===================================================================*/
 /* NRDF D1594 Data No.10                                             */
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 /* Bibliography                                                      */
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 \\BIB,10;
 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,10;
 /* 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         unpublished.]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=208PB(3HE,3HE)208PB;
 PHQ=ANGL-DSTRN;
 ENR=>99%'51';
 /* '51' Larger than 99% for thick target while unknown for thin
         target */
 THK-TGT=(58.0MG/CM**2, 8.6MG/CM**2)'52';
 /* '52' Thin target (8.6 mg/cm**2) was used for measurement at
         forward-scattering angle */
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 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,10;
 INC-ENGY-LAB=450MEV;
 SYS-ERR=15%'53';
 /* '53' 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'54';
 /* '54' Overall angular resolution */
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 THTC DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA'55'
 (DEG) (MB/SR) (MB/SR)
 6.4 1330. +-10.
 6.9 1610. +-10.
 7.4 1094. +-11.
 7.9 487. +-0.9
 8.4 62.4 +-1.3
 8.9 81.9 +-1.3
 9.4 159. +-2.0
 9.9 162. +-2.0
 10.4 57.0 +-0.9
 10.9 11.1 +-0.4
 11.4 7.33 +-0.33
 11.9 18.5 +-0.5
 12.5 21.7 +-0.5
 13.0 10.6 +-0.2
 13.5 3.08 +-0.14
 14.0 1.17 +-0.09
 14.5 3.59 +-0.06
 15.0 3.73 +-0.06
 15.5 2.52 +-0.05
 16.0 1.22 +-0.03
 16.5 0.321 +-0.034
 17.0 0.434 +-0.040
 17.5 0.537 +-0.044
 18.0 0.481 +-0.042
 18.6 0.217 +-0.009
 19.1 0.0807 +-0.006
 19.6 0.0635 +-0.005
 20.1 0.0783 +-0.006
 20.6 0.0844 +-0.004
 21.1 0.0497 +-0.003
 21.6 0.0323 +-0.003
 22.1 0.0141 +-0.002
 22.6 0.0134 +-0.0017
 23.1 0.0140 +-0.0017
 23.6 0.0140 +-0.0017
 24.1 0.00938 +-0.0014
 25.7 0.00432 +-0.0008
 26.2 0.00256 +-0.0006
 26.7 0.000957 +-0.0004
 27.2 0.000957 +-0.0004
 27.7 0.00028 +-0.0002
 28.2 0.00028 +-0.0002
 29.2 0.00014 +-0.00014
 \END;
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