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 /* NRDF D1718 Data No.2                                              */
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 /* Bibliography                                                      */
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 \\BIB,2;
 D#=D1718;
 TITLE=/ Polarization transfer and spin response function in
         quasielastic (p,n) reactions at 346 MeV /;
 ATH=(T.WAKASA'1', H.SAKAI'1', K.HATANAKA'2', H.OKAMURA'1', H.OTSU'1',
      S.FUJITA'1', T.NONAKA'1', T.UESAKA'1', Y.SATOU'1', T.OHNISHI'1',
      G.YOKOYAMA'1', S.ISHIDA'3', N.SAKAMOTO'3', M.B.GREENFIELD'4',
      M.ICHIMURA'1', K.KAWAHIGASHI'5');
 INST-ATH=(2JPNTOK'1', 2JPNRCN'2', 2JPNIPC'3', 2JPNICU'4',
           2JPNJPN'5');
      /* '1' Department of Physics */
      /* '4' Division of Natural Science */
      /* '5' Dept. of Information Science, Kanagawa Univ., Hiratsuka
 REF=(PR/C'6');
 VLP=(59(1999)3177'6');
 /* Secondary reference 
    - NP/A, 631(1998)757 (H.Sakai et al., Proceedings of the XVth
      International Conference on Few-Body Problems in Physics
      (Groningen, 1997))
 RCTS=(D(P,N)X, 6LI(P,N)X, 12C(P,N)X, 40CA(P,N)X, 208PB(P,N)X);
 PHQS=(ENGY-SPEC, POL, VCTR-ANALPW, POL-TRNSF'7', POL-TRNSF'8',
       POL-TRNSF'9', POL-TRNSF'10', POL-TRNSF'11', POL-TRNSF'12');
 /* '7' Polarization transfer coefficient, D(S,S') */
 /* '8' Polarization transfer coefficient, D(S',L). See Eq.(1) in
    reference. */
 /* '9' Polarization transfer coefficient, D(N,N). See Eq.(1) in
    reference. */
 /* '10' Polarization transfer coefficient, D(L',S). See Eq.(1) in
    reference. */
 /* '11' Polarization transfer coefficient, D(L',L). See Eq.(1) in
    reference. */
 /* '12' Polarization transfer coefficient, D(S',S). See Eq.(1) in
    reference. */
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 /* Experimental Conditions                                           */
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 \\EXP,2;
 /* 2001-09-20 : Converted, Ay + On. Converted to EXFOR E1718 */
 /* 2002-07-04 : Altered, On */
 /* 2004-07-21 : Altered, On. INSTITUTE corrected. Additional
    references and METHOD added. */
 RTY=POL-RCT;
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=CYC;
 INST-ACC=2JPNRCN;
 INC-ENGY-LAB=346MEV;
 ION-SOURCE=/ Polarized ion source (High intensity polarized ion source
              (HIPIS), See [K.Hatanaka et al., Nucl.Instrum
              Method.Phys.Res.A384(1997)575].) /;
 DET-PARTCL=N;
 COINC=NO;
 ANT-COINC=NO;
 DET-SYS=(MAG,SCT'13',SCT'14',TOF'15');
 /* '13' Plastic scintillator NPOL2, See [T.Wakasa et al.,
         Nucl.Instrum.Methods Phys.A404(1998)355]. */
 /* '14' Liquid scintillator */
 /* '15' To measure neutron energy */
 ERS-DET=XMEV'16';
 /* '16' 2 and 3 MeV for cross section and polarization transfer
         measurement, respectively. */
 MONTR-RCT=/ , The beam polarizations (S,N,L) were monitored with two
             beam-line polarimeters BLP1 and BLP2. These polarimeters
             are separated by a bend angle of 98deg, thus the
             horizontal and vertical components of the polarization
             vector can be determined simultaneously. Each polarimeter
             consists of four arms of collimated pairs of
             confugate-angle plastic-scintillator telescopes. The
             polarimetry is based on the analyzing power of the
             1H(p,p)1H scattering. /;
 /* Experimental Method:
    - Time-of-flight (To measure neutron energy)
    - Double scattering (To measure neutron polarization)
 RCT=6LI(P,N)X;
 PHQ=ENGY-SPEC;
 ENR=>99%;
 CHM=ELM;
 PHYS-FORM=SLD;
 THK-TGT=181MG/CM**2;
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 /* Descriptive Parameters                                            */
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 \\DATA,2;
 INC-ENGY-LAB=346MEV;
 THTL=22DEG;
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 /* Data Table                                                        */
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 \DATA;
 TRNSF-ENGY'18' DSIGMA/DOMEGA/DE DELTA-DSIGMA/DOMEGA/DE
 (MEV) (MB/SR/MEV) (MB/SR/MEV)
 25.0 0.0889 +-0.0003
 30.0 0.1265 +-0.0003
 35.0 0.2009 +-0.0004
 40.0 0.3045 +-0.0005
 45.0 0.3813 +-0.0006
 50.0 0.4279 +-0.0006
 55.0 0.4577 +-0.0007
 60.0 0.4759 +-0.0007
 65.0 0.4794 +-0.0007
 70.0 0.4720 +-0.0007
 75.0 0.4533 +-0.0007
 80.0 0.4279 +-0.0006
 85.0 0.3934 +-0.0006
 90.0 0.3601 +-0.0006
 95.0 0.3258 +-0.0006
 100.0 0.2926 +-0.0005
 105.0 0.2649 +-0.0005
 110.0 0.2369 +-0.0005
 115.0 0.2140 +-0.0004
 120.0 0.1943 +-0.0004
 125.0 0.1757 +-0.0004
 130.0 0.1607 +-0.0004
 135.0 0.1480 +-0.0004
 140.0 0.1361 +-0.0004
 145.0 0.1267 +-0.0003
 150.0 0.1190 +-0.0003
 155.0 0.1115 +-0.0003
 160.0 0.1058 +-0.0003
 165.0 0.1011 +-0.0003
 170.0 0.0975 +-0.0003
 175.0 0.0929 +-0.0003
 180.0 0.0902 +-0.0003
 185.0 0.0880 +-0.0003
 190.0 0.0857 +-0.0003
 195.0 0.0845 +-0.0003
 200.0 0.0832 +-0.0003
 \END;
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