/*===================================================================*/
 /* NRDF D1986 Data No.2                                              */
 /*===================================================================*/
 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,2;
 D#=D1986;
 TITLE=/ Measurement of neutron emission spectra in Li(d,xn) reaction
         with thick and thin targets for 40-MeV deuterons /;
 ATH=(M.HAGIWARA'1', T.ITOGA'1', N.KAWATA'1', N.HIRABAYASHI'1',
      T.OISHI'1', T.YAMAUCHI'1', M.BABA'1', M.SUGIMOTO'2',
      T.MUROGA'3');
 INST-ATH=(2JPNTOH'1', 2JPNJAE'2', 2JPNNIF'3');
      /* '1' Cyclotron and Radioisotope Center */
 REF=FST;
 VLP=48(2005)1320;
 RCTS=LI(D,N)X;
 PHQS=(TTY, DBL-DIFF-XSECTN);
 /*===================================================================*/
 /* Experimental Conditions                                           */
 /*===================================================================*/
 \\EXP,2;
 /* 2006-05-30 : Recieved, On. Received by e-mail from M.Hagiwara
 /* 2006-05-31 : Compiled, Kc + On */
 /* Additional results shown but not compiled
    - Neutron spectra (Neutron energy spectra from thin lithium
      target (Fig.10, p1326 in reference))
 ENR=NAT;
 CHM=ELM;
 PHYS-FORM=SLD;
 THK-BAC=XMG/CM**2'4';
 /* '4' 30-mm diameter x 21.4-mm thickness (thick target) and 30-mm
        diameter x 0.86-mm thickness (thin target) */
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=CYC'5';
 /* '5' Isochronous cyclotron, AVF cyclotron */
 INST-ACC=2JPNTOH'6';
 /* '6' Cyclotron and Radioisotope Center */
 BEAM-INTNSTY=0.1[20NA;
 POL-PRJ=0%;
 DET-PARTCL=N;
 COINC=NO;
 ANT-COINC=NO;
 DET-SYS=(SCT'7',TOF'8');
 /* '7' To detect neutrons emitted from targets (NE213) */
 /* '8' Flight path of 11/3.45 m for high/low energy region */
 SOLID-ANGL=<0.17MSR;
 /* Correction were performed for the effects of (a) neutron
    attenuation in target and (b) neutron attenuation in the air and
    the wall of target chamber. */
 /* Related references 
    - common, none, J(Nucl)145.
    . See also EXFOR commo.n.
 RCT=LI(D,N)X;
 PHQ=TTY;
 INC-ENGY-LAB=40MEV;
 ANL=MONTE-MTHD'15';
 /* '15' Monte Carlo codes McDeLi, McDeLicious and MCNPX */
 /* Analysis:
    - Integration of energy distribution (Assuming the flat spectrum
      below 1 MeV. Uncertainty due to the assumption of the flat
      spectrum below 1 MeV is not significant (<1%).)
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,2;
 TOT-ERR=X%'9';
 /* '9' Total normalization uncertainties are generally several
        percent but are 15 to 25% at the highest energy (>40 MeV)
        because of the statistical uncertainties. */
 SYS-ERR=(6%'10',<10%'11');
 /* '10' Uncertainty of detector efficiency with the SCINFUL-R
         code */
 /* '11' Maximum uncertainty of attenuation in target (larger at
         backward angles and ranged up to 20% at low energy (<8 MeV)
         and generally several percent for the air and chamber wall.)
 STATIST-ERR=<10%'12';
 /* '12' Maximum statistical uncertainty (larger than 20% at the
         highest energy (>40 MeV)) */
 INC-ENGY-LAB=40MEV;
 DELTA-THTL=0.5DEG'16';
 /* '16' Upper limit of angular resolution */
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 THTL TTY DELTA-TTY
 (DEG)
 0 4.48E+11 +-4.72E+10
 10 1.69E+11 +-1.84E+10
 15 1.07E+11 +-1.20E+10
 20 8.94E+10 +-1.04E+10
 30 6.26E+10 +-7.59E+09
 45 4.40E+10 +-5.95E+09
 60 2.74E+10 +-3.71E+09
 90 1.62E+10 +-1.44E+09
 110 1.24E+10 +-2.04E+09
 \END;
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