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 /* NRDF D1618 Data No.1                                              */
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 /* Bibliography                                                      */
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 \\BIB,1;
 D#=D1618;
 TITLE=/ Medium energy gamma rays following radiative capture of 50
         MeV polarized protons on 11B /;
 PURPOSE=/ This report aims at presenting the analyzing power
           measurement of medium energy gamma rays following radiative
           caputure of 50 MeV polarized protons and at showing the
           dependence of the analyzing power on the spin direction of
           the captured proton. /;
 ATH=(M.NOMACHI'1', T.SHIBATA'1', K.OKADA'1', T.MOTOBAYASHI'1',
      F.OHTANI'1', H.EJIRI'1', T.KISHIMOTO'2');
 INST-ATH=(2JPNOSA'1', 2JPNTIT'2');
      /* '1' Department of Physics and Laboratory of Nuclear Studies
      /* '2' Department of Physics */
 REF=PR/C;
 VLP=31(1985)242;
 RCTS=11B(P,GAMMA)12C;
 PHQS=(ANGL-DSTRN, ANGL-DSTRN'3', VCTR-ANALPW);
 /* '3' Legendre Coefficient */
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 /* Experimental Conditions                                           */
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 \\EXP,1;
 /* 2003-10-01 : Converted, Sr + Am + On. Converted to EXFOR E1618
 RTY=POL-RCT;
 ENR=98.6%;
 CHM=ELM;
 PHYS-FORM=SLD;
 THK-TGT=31MG/CM**2;
 BAC=SELF;
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=CYC;
 INST-ACC=2JPNRCN;
 INC-ENGY-LAB=50MEV;
 BEAM-INTNSTY=15[30NA;
 POL-PRJ=70[75%;
 DET-PARTCL=GAMMA;
 COINC=NO;
 ANT-COINC=NO;
 DET-SYS=(NAI'4',SCT'5',TOF'6');
 /* '4' NaI crystal ensemble called HERMES [T.Kishimoto, et al.,
        Nucl.Instrum.Methods 198(1982)269] */
 /* '5' Plastic scintillator shield as a Compton suppressor */
 /* '6' To separate gamma rays from neutrons */
 ERS-DET=3.8%'7';
 /* '7' The overall resolution for 60 MeV gamma rays was about 3.8%
        (delta-E/E), including 1% due to the target thickness. */
 /* 2006-12-19 : Altered, At. Re-digitized */
 RCT=11B(P,GAMMA)12C;
 PHQ=ANGL-DSTRN;
 ANL=X'8';
 /* '8' Calculation given in Refs. [S.F.Tsai et al., Phys. Rev.
        Lett. 43(1979)576] and [M.Gari et al., Phys. Rev.
        C18(1978)1071] in terms of both the one-body and the two-body
        direct processes */
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 /* Descriptive Parameters                                            */
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 \\DATA,1;
 INC-ENGY-LAB=50MEV;
 SYS-ERR=[25%'9';
 /* '9' The systematic error for the absolute cross sections due to
        the target thickness, the efficiency of the HERMES, and the
        beam current integration amouts to about 25%. */
 EXC-ENGY=0.0MEV;
 J-PTY=0+;
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 /* Data Table                                                        */
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 \DATA;
 THTC DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA
 (DEG) (NB/SR) (NB/SR)
 4.045E+01 1.760E+02 +-NEGLIGIBLE
 6.080E+01 1.647E+02 +-1.928E+01
 8.094E+01 9.694E+01 +-9.385E+00
 1.113E+02 2.284E+01 +-3.026E+00
 \END;
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