DARPE: Search Results
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 /* NRDF D1845 Data No.7                                              */
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 /* Bibliography                                                      */
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 \\BIB,7;
 D#=D1845;
 TITLE=/Feshbach-Kerman-Koonin model analysis of preequilibrium (p,p')
        and (p,n) reactions at 12 to 26 MeV/;
 PURPOSE=/To investigate preequilibrium nucleon emission in the low
          incident energy region below 30 MeV/;
 ATH=(Y.WATANABE'1', A.AOTO'1', H.KASHIMOTO'1', S.CHIBA'2',
      T.FUKAHORI'2', K.HASEGAWA'2', M.MIZUMOTO'2', S.MEIGO'2',
      M.SUGIMOTO'2', Y.YAMANOUTI'2', N.KOORI'3', M.B.CHADWICK'4',
      P.E.HODGSON'5');
 INST-ATH=(2JPNKYU'1', 2JPNJAE'2', 2JPNTKS'3', 1USALRL'4', 2UK OXF'5');
      /* '1' Department of Energy Conversion Engineering */
      /* '3' Faculty of Integrated Arts and Sciences */
      /* '4' Nuclear Data Group */
      /* '5' Nuclear Physics Laboratory, Physics Department */
 REF=PR/C;
 VLP=51(1995)1891;
 RCTS=(98MO(P,P)X, 106PD(P,P)X);
 PHQS=ENGY-SPEC;
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 /* Experimental Conditions                                           */
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 \\EXP,7;
 /* 2003-11-13 : Converted, Data converted from EXFOR O0558 */
 CHM=ELM;
 PHYS-FORM=SLD'6';
 /* '6' metalic foils */
 BAC=SELF;
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=VDGT;
 INST-ACC=2JPNJAE;
 BEAM-INTNSTY=XNA'7';
 /* '7' Beam current was adjusted in a range from about several
        tens of nA to about 300 nA in accordance with the detector
        angle. */
 POL-PRJ=0%;
 DET-PARTCL=P;
 COINC=NO;
 ANT-COINC=NO;
 DET-SYS=SBD'8';
 /* '8' as Delta E-E counter to detect all emitted charged
        particles separately and suppress background events due to
        gamma-rays. */
 ANL=X'9';
 /* '9' Multistep direct (MSD) and multistep-compound (MSC)
        reaction models of Feshbach, Kerman, and Koonin (FKK) using the
        FKK-GNASH code [M.B.Chadwick and P.G.Young, Phys. Rev. C47
        (1993) 2255] */
 /* Experimental Method:
    - Particle identification by 'E/Delta E' measurement (To detect
      all emitted charged particles separately and suppress background
      events due to gamma-rays)
    - Beam current integrated (Beam intensity was monitored by means
      of a current integrator connected to a Faraday cup and the beam
      current was adjusted in a range from about several tens of nA to
      about 300 nA in accordance with the detector angle.)
 RCT=98MO(P,P)X;
 PHQ=ENGY-SPEC;
 ENR=97.1%;
 THK-TGT=0.45MG/CM**2;
 INC-ENGY-LAB=25.6MEV;
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 /* Descriptive Parameters                                            */
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 \\DATA,7;
 INC-ENGY-LAB=25.6MEV;
 SYS-ERR=<8%'38';
 /* '38' Absolute uncertainty involved in the normalization */
 NORM=/ Elastic cross sections at small angles are normalized to the
        optical model prediction /;
 EMT=P;
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 /* Data Table                                                        */
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 \DATA;
 ENGY-EMT-LAB DELTA-DSIGMA/DE
 (MEV) (MB/MEV)
 \END;
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