DARPE: Search Results
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 /* NRDF D1760 Data No.17                                             */
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 /* Bibliography                                                      */
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 \\BIB,17;
 D#=D1760;
 TITLE=/SPALLATION NEUTRON MEASUREMENT BY THE TIME-OF-FLIGHT METHOD
        WITH A SHORT FLIGHT PATH/;
 PURPOSE=/TO MEASURE THE DOUBLE DIFFERENTIAL CROSS SECTION ON PRODUCTION
          OF THE SPALLATION NEUTRONS./;
 ATH=(T.NAKAMOTO'1', K.ISHIBASHI'1', N.MATSUFUJI'1', N.SHIGYO'1',
      K.MAEHATA'1', S.MEIGO'2', H.TAKADA'2', S.CHIBA'2',
      M.NUMAJIRI'3', T.NAKAMURA'4', Y.WATANABE'5');
 INST-ATH=(2JPNKYU'1', 2JPNJAE'2', 2JPNLEP'3', 2JPNTOH'4', 2JPNKYU'5');
      /* '1'DEPARTMENT OF NUCLEAR ENGINEERING */
      /* '4'CYCLOTRON RADIOISOTOPE CENTER */
      /* '5'ENERGY CONVERSION ENGINEERING */
 REF=NST;
 VLP=32(1995)827;
 RCTS=(C(P,N)X, PB(P,N)X);
 PHQS=ENGY-SPEC;
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 /* Experimental Conditions                                           */
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 \\EXP,17;
 /* 2002-11-15 : COMPILED, AUTHOR (T.NAKAMOTO) RECOMMEND TO USE
    DATA SET IN OTHER REFERENCE [NUCL.SCI.TECHNOL.34(1997)529]. */
 RTY=SPAL;
 PHQ=ENGY-SPEC;
 ENR=NAT;
 CHM=ELM;
 PHYS-FORM=SLD;
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=SYN'6';
 /* '6' THE PI-2 LINE OF THE 12 GEV PROTON SYNCHROTRON */
 INST-ACC=2JPNLEP;
 BEAM-INTNSTY=XMA'7';
 /* '7' IN A LEVEL OF 100000 PROTONS / 2.5 S AT THE PI-2 BEAM LINE. */
 POL-PRJ=0%;
 ION-SOURCE=/ INCIDENT PROTONS WERE GENERATED AS SECONDARY BEAM. TOF
              METHOD WITH A PAIR OF PILOT U SCINTILLATORS WAS ADOPTED
              FOR SEPARATION BETWEEN PROTONS AND PIONS. /;
 DET-PARTCL=N;
 COINC=NO;
 ANT-COINC=NO;
 DET-SYS=(TOF,SCT'8',PLST-SCT'9');
 /* '8' TWO DEFFERENT SIZES (DIAMETERXTHICK=5CMX5CM, 2CMX2CM) OF NE213
    NEUTRON DETECTORS WERE PLACED IN THE DIRECTIONS OF 15 DEGREE, 30
    DEGREE, 60 DEGREE, 90 DEGREE, 120 DEGREE AND 150 DEGREE */
 /* '9' NE102A PLASTIC SCINTILLATORS WERE MOUNTED AS VETO DETECTORS TO
    ELIMINATE CHARGED PARTICLE EVENTS BY THE ANTI-COINCIDENCE METHOD
 ERS-DET=XKEV'10';
 /* '10' THE ENERGY RESOLUTIONS IN ONE SIGMA WERE 5.7 % AT THE NEUTRON
    ENERGY OF 10 MEV AND 14 % AT 300 MEV. */
 EFCN-DET=/ THE UNCERTAINTY OF THE NEUTRON DETECTION EFFICIENCY RANGED
            UP TO 10 % /;
 RCT=PB(P,N)X;
 THK-TGT=15000MG/CM**2;
 INC-ENGY-LAB=1.5GEV;
 DET-PARTCL=N;
 ANL=MONTE-MTHD'19';
 /* '19' HETC (HIGH ENERGY TRANSPORT CODE) [K.C.CHANDLER,
    T.W.ARMSTRONG, CCC-178(1977)]. */
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 /* Descriptive Parameters                                            */
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 \\DATA,17;
 INC-ENGY-LAB=1.5GEV;
 EMT=N;
 THTL=60DEG;
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 /* Data Table                                                        */
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 \DATA;
 ENGY-EMT-LAB DSIGMA/DOMEGA/DE DELTA-DSIGMA/DOMEGA/DE
 (MEV) (B/SR/MEV) (B/SR/MEV)
 1.2500 0.30913    +-0.088686
 1.7500 0.27736    +-0.071239
 2.5000 0.23144    +-0.052895
 3.5000 0.17440    +-0.035927
 4.5000 0.13452    +-0.025250
 5.5000 0.099326   +-0.017266
 7.0000 0.060781   +-0.0096187
 9.0000 0.061966   +-0.0089827
 12.500 0.034741   +-0.0046439
 17.500 0.016509   +-0.0022092
 25.000 0.012760   +-0.0015980
 35.000 0.0089780  +-0.0011772
 45.000 0.0080174  +-0.0010986
 55.000 0.0069350  +-0.0010221
 70.000 0.0060827  +-0.00080414
 90.000 0.0036406  +-0.00058688
 125.00 0.0020199  +-0.00029940
 175.00 0.0010126  +-0.00019786
 250.00 0.00046622 +-9.7718E-05
 350.00 0.00010240 +-4.6150E-05
 450.00 0.00016134 +-4.7561E-05
 550.00 8.5853E-05 +-4.1121E-05
 \END;
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