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 /* NRDF D1893 Data No.8                                              */
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 /* Bibliography                                                      */
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 \\BIB,8;
 D#=D1893;
 TITLE=/ Measurements of differential thick target neutron yields and
         7Be production in the Li, 9Be(d,n) reactions for 25 MeV
         deuterons /;
 PURPOSE=/ To know the production of radioactivity in lithium target
           under deuteron bombardment /;
 ATH=(T.AOKI'1', M.HAGIWARA'1', M.BABA'1', M.SUGIMOTO'2', T.MIURA'1',
      N.KAWATA'1', A.YAMADERA'1');
 INST-ATH=(2JPNTOH'1', 2JPNJAE'2');
 REF=NST;
 VLP=41(2004)399;
 /* Secondary references 
    - 2004SANTA, (2004)884 (Same Li(d,x)7Be thick target yield given)
    - JNM, 307-311(2002)1715 (Preliminary report on 7Li(d,xn))
 RCTS=(LI(D,)X, 7LI(D,)X, 9BE(D,)X, LI(D,)7BE, 9BE(D,)7BE);
 PHQS=(N-MLT, TTY);
 /*===================================================================*/
 /* Experimental Conditions                                           */
 /*===================================================================*/
 \\EXP,8;
 /* 2004-05-08 : Compiled+Checked, Kc + On */
 /* 2020-07-07 : Altered, Tada. Secondary reference add. Reference
    modified. */
 /* 2022-01-19 : Altered, On. Major revisions in 002-022. */
 /* 2023-04-16 : Altered, MA. REACTION in 022 was modified. */
 PHYS-FORM=X'4';
 /* '4' Metallic plate */
 THK-TGT=XMG/CM**2'5';
 /* '5' about 7.5 mm (Li) and about 3 mm (Be) to stop the incident
        beam within target targets */
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=CYC'6';
 /* '6' Isochronous cyclotron, K=110 MeV AVF cyclotron */
 INST-ACC=2JPNTOH'7';
 /* '7' Cyclotron and Radioisotope Center */
 BEAM-INTNSTY=<5NA;
 POL-PRJ=0%;
 COINC=NO;
 ANT-COINC=NO;
 DET-SYS=(SCT'8',HPGE'9');
 /* '8' To detect neutron (NE213). Efficiency curves were obtained
        by revised version of Monte Carlo Code SCINFUL [J.K.Dickens,
        ORNL-6436, Oak Ridge National Laboratory, 1988]. */
 /* '9' To analyze gamma ray from target (EURICIS MESURESE
        GPC50-195-R, 50% efficiency). Efficiency was determined by
        Monte Carlo Code EGS4 [W.Nelson et al., SLAC-265, Stanford
        University, Stanford, 1985]. */
 RCT=7LI(D,)X;
 PHQ=N-MLT;
 DET-PARTCL=N;
 DET-SYS=TOF;
 /* Experimental Method:
    - Beam current integrated (To normalize spectra)
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 /* Descriptive Parameters                                            */
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 \\DATA,8;
 SYS-ERR=5%'26';
 /* '26' Uncertainty in efficiency */
 THTL=40DEG;
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 /* Data Table                                                        */
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 \DATA;
 ENGY-EMT-LAB DN/DOMEGA/DE DELTA-DN/DOMEGA/DE'27'
 (MEV) (1/SR/MEV/UCOULOMB) (1/SR/MEV/UCOULOMB)
 1.00E+00 3.77E+09 +-3.12E+08
 1.10E+00 3.47E+09 +-2.87E+08
 1.20E+00 3.31E+09 +-2.74E+08
 1.30E+00 3.15E+09 +-2.61E+08
 1.40E+00 3.09E+09 +-2.56E+08
 1.50E+00 2.93E+09 +-2.43E+08
 1.60E+00 2.89E+09 +-2.40E+08
 1.70E+00 2.76E+09 +-2.29E+08
 1.80E+00 2.66E+09 +-2.20E+08
 1.90E+00 2.65E+09 +-2.19E+08
 2.00E+00 2.59E+09 +-2.14E+08
 2.10E+00 2.50E+09 +-2.07E+08
 2.20E+00 2.48E+09 +-2.06E+08
 2.30E+00 2.43E+09 +-2.01E+08
 2.40E+00 2.41E+09 +-1.99E+08
 2.50E+00 2.38E+09 +-1.97E+08
 2.60E+00 2.35E+09 +-1.94E+08
 2.70E+00 2.34E+09 +-1.94E+08
 2.80E+00 2.26E+09 +-1.88E+08
 2.90E+00 2.26E+09 +-1.87E+08
 3.00E+00 2.20E+09 +-1.82E+08
 3.10E+00 2.20E+09 +-1.83E+08
 3.20E+00 2.22E+09 +-1.84E+08
 3.30E+00 2.20E+09 +-1.83E+08
 3.40E+00 2.21E+09 +-1.83E+08
 3.50E+00 2.13E+09 +-1.77E+08
 3.60E+00 2.11E+09 +-1.75E+08
 3.70E+00 2.06E+09 +-1.71E+08
 3.80E+00 2.07E+09 +-1.72E+08
 3.90E+00 2.06E+09 +-1.71E+08
 4.00E+00 2.05E+09 +-1.71E+08
 4.10E+00 2.03E+09 +-1.69E+08
 4.20E+00 2.06E+09 +-1.71E+08
 4.30E+00 1.98E+09 +-1.65E+08
 4.40E+00 1.93E+09 +-1.61E+08
 4.50E+00 1.92E+09 +-1.60E+08
 4.60E+00 1.87E+09 +-1.55E+08
 4.70E+00 1.80E+09 +-1.50E+08
 4.80E+00 1.76E+09 +-1.47E+08
 4.90E+00 1.70E+09 +-1.41E+08
 5.00E+00 1.63E+09 +-1.36E+08
 6.00E+00 1.51E+09 +-1.25E+08
 7.00E+00 1.33E+09 +-1.10E+08
 8.00E+00 1.17E+09 +-9.68E+07
 9.00E+00 1.01E+09 +-8.33E+07
 1.00E+01 8.69E+08 +-7.16E+07
 1.10E+01 7.09E+08 +-5.85E+07
 1.20E+01 6.01E+08 +-4.96E+07
 1.30E+01 5.02E+08 +-4.15E+07
 1.40E+01 3.99E+08 +-3.30E+07
 1.50E+01 3.13E+08 +-2.59E+07
 1.60E+01 2.49E+08 +-2.06E+07
 1.70E+01 2.01E+08 +-1.67E+07
 1.80E+01 1.50E+08 +-1.25E+07
 1.90E+01 1.19E+08 +-9.96E+06
 2.00E+01 9.97E+07 +-8.34E+06
 2.10E+01 7.20E+07 +-6.06E+06
 2.20E+01 5.99E+07 +-5.05E+06
 2.30E+01 5.53E+07 +-4.67E+06
 2.40E+01 5.18E+07 +-4.39E+06
 2.50E+01 4.59E+07 +-3.90E+06
 2.60E+01 4.17E+07 +-3.55E+06
 2.70E+01 3.95E+07 +-3.38E+06
 2.80E+01 3.71E+07 +-3.17E+06
 2.90E+01 3.76E+07 +-3.22E+06
 3.00E+01 3.73E+07 +-3.19E+06
 3.10E+01 3.62E+07 +-3.10E+06
 3.20E+01 3.72E+07 +-3.19E+06
 3.30E+01 3.35E+07 +-2.88E+06
 3.40E+01 2.81E+07 +-2.44E+06
 3.50E+01 1.89E+07 +-1.68E+06
 3.60E+01 1.19E+07 +-1.10E+06
 3.70E+01 7.16E+06 +-7.11E+05
 3.80E+01 2.70E+06 +-3.31E+05
 3.90E+01 6.21E+05 +-1.34E+05
 4.00E+01 1.38E+05 +-6.88E+04
 4.10E+01 1.20E+05 +-6.60E+04
 4.20E+01 1.34E+05 +-6.87E+04
 \END;
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