DARPE: Search Results
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 /* NRDF D1808 Data No.1                                              */
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 /* Bibliography                                                      */
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 \\BIB,1;
 D#=D1808;
 TITLE=/Characterization of a 40-90 MeV 7Li(p,n) neutron source at
        TIARA using a proton recoil telescope and a TOF method/;
 PURPOSE=/The purpose of this experiment is to measure the intensity
          and the spectrum of neutron source produced by 7Li(p,n)
          reaction with PRT and TOF methods./;
 ATH=(M.BABA'1', Y.NAUCHI'1', T.IWASAKI'1', T.KIYOSUMI'1',
      M.YOSHIOKA'1', S.MATSUYAMA'1', N.HIRAKAWA'1', T.NAKAMURA'2',
      SU.TANAKA'3', S.MEIGO'1', H.NAKASHIMA'4', SH.TANAKA'5',
      N.NAKAO'6');
 INST-ATH=(2JPNTOH'1', 2JPNTOH'2', 2JPNJAE'3', 2JPNJAE'4', 2JPNJAE'5',
           2JPNKEK'6');
      /* '1' Graduate School of Quantum Science & Energy Engineering */
      /* '2' Cyclotron Radioisotope Center */
      /* '3' Takasaki Establishment */
      /* '4' Tokai Establishment */
      /* '5' Planning Office */
      /* '6' Tanashi Branch */
 REF=NIM/A;
 VLP=428(1999)454;
 RCTS=7LI(P,N)7BE;
 PHQS=XSECTN'7';
 /* '7' The 0-degree cross section for the peak neutron production
    was deduced from the present data by integration of the spectra
    over the peak area. */
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 /* Experimental Conditions                                           */
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 \\EXP,1;
 /* 2004-06-07 : Compiled */
 /* Additional result not compiled:
    - Energy distribution (Energy distribution of neutron (shown by
      continuous lines in the reference and unobtainable from author))
 ENR=99.8%;
 CHM=ELM;
 PHYS-FORM=SLD'8';
 /* '8' Target is a rolled plate of metallic 7Li, 35-mm diameter.
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=CYC'9';
 /* '9' Isochronous cyclotron, K=110 AVF cyclotron of TIARA */
 INST-ACC=2JPNJAE'10';
 /* '10' Takasaki Establishment */
 POL-PRJ=0%;
 DET-PARTCL=N;
 COINC=NO;
 ANT-COINC=NO;
 RCT=7LI(P,N)7BE;
 RTY=KNOCK'11';
 /* '11' 7Li(p,n)7Be */
 PHQ=XSECTN'12';
 /* '12' The 0-degree cross section for the peak neutron
         production was deduced from the present data by integration of
         the spectra over the peak area. */
 THK-TGT=XMG/CM**2'13';
 /* '13' Target thicknesses 3.60, 3.80, 4.30, 4.70, 5.00, 5.20,
         6.00, 6.75 mm are for the incident proton eneryg Ep=43, 48,
         53, 58, 63, 68, 78 and 87 MeV, respectively. */
 INC-ENGY-LAB=43[87MEV;
 DET-SYS=(NAI'14',SI'15',SCT'16',TOF);
 /* '14' Used as E counter to measure recoil proton in PRT method
 /* '15' Used as dE counter to measure recoil proton in PRT method
 /* '16' Organic scintillator (BC501A, NE213) used as TOF counter
 /* Experimental Method:
    - PRT (Proton Recoil Telescope method)
    - Time-of-flight
 /* Analysis:
    - Integration of energy distribution (Integration of the spectra
      over the peak area)
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 /* Descriptive Parameters                                            */
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 \\DATA,1;
 RSD=7BE;
 THTL=0DEG;
 EXC-ENGY=(0.0MEV,0.431MEV)'17';
 /* '17' Deduced from Q-values given in p458 of the reference */
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 /* Data Table                                                        */
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 \DATA;
 INC-ENGY-LAB DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA
 (MEV) (MB/SR) (%)
 43   35.0   +-3.4
 48   29.8   +-3.3
 53   33.4   +-4.7
 58   34.6   +-3.6
 63   33.8   +-3.5
 68   33.9   +-3.9
 78   35.5   +-4.5
 87   35.1   +-6.2
 \END;
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