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 /* NRDF D1594 Data No.13                                             */
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 /* Bibliography                                                      */
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 \\BIB,13;
 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);
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 /* Experimental Conditions                                           */
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 \\EXP,13;
 /* 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         unpublished.]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         ECIS88, unpublished.]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=OPT-POTL-PARA;
 ENR=>99%'64';
 /* '64' Enrichment is larger than 99% for thick target while
         unknown for thin target */
 THK-TGT=(52.0MG/CM**2, 5.9MG/CM**2)'65';
 /* '65' Thin target (5.9mg/cm**2) was used for measurement at
         forward-scattering angle */
 /* Comment to data: In the third line of original table (Table 1) in
    reference, 56Ni is assigned as target nucleus, however this is
    probably misprint */
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 /* Descriptive Parameters                                            */
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 \\DATA,13;
 INC-ENGY-LAB=450MEV;
 SYS-ERR=15%'66';
 /* '66' 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'67';
 /* '67' Overall angular resolution */
 POTL-FORM=/ Uc(X)
             -V*f(X,Rr,Ar)
             -i*W*f(X,Riv,Aiv)
            : Uniform charge of radius Rc*A**(1/3)
            : f(X,R,A)=1/(1+exp((X-R*A**(1/3))/A)
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 /* Data Table                                                        */
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 \DATA;
 V RR AR WV RIV AIV RC DATA1'68'
 (MEV) (FM) (FM) (MEV) (FM) (FM) (FM) (NODIM)
 29.8 1.34 0.83 59.8 0.67 1.19 20.8
 \END;
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