/*===================================================================*/
 /* NRDF D1870 Data No.2                                              */
 /*===================================================================*/
 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,2;
 D#=D1870;
 TITLE=/ On the neutrons from the 14N(d,n)15O reaction - II /;
 PURPOSE=/ To extend the measured angular range of our previous work
           on 14N(d,n)15O reaction to the more backward direction /;
 ATH=(I.NONAKA'1', S.MORITA'1', N.KAWAI'1', T.ISHIMATSU'1',
      K.TAKESHITA'1', Y.NAKAJIMA'1', N.TAKANO'1');
 INST-ATH=(2JPNKYU'1');
      /* '1' Department of Physics, Faculty of Science */
 REF=JPJ;
 VLP=12(1957)841;
 RCTS=(2H(D,N)3HE, 14N(D,N)15O);
 PHQS=(ANGL-DSTRN, XSECTN);
 /*===================================================================*/
 /* Experimental Conditions                                           */
 /*===================================================================*/
 \\EXP,2;
 /* 2004-02-19 : Compiled, Sr + On */
 /* Related references 
    - J.L.Fowler et al., RMP, 28(1956)103.
    Reference for monitor (Angular distribution for 2H(d,n)3He given in
    Fig.16, p112 of this reference)
 CHM=X'2';
 /* '2' Deuterium gas mixed to nitrogen gas */
 PHYS-FORM=GAS;
 THK-TGT=XMG/CM**2'3';
 /* '3' Pressures of deuterium gas and nitrogen gas are 4.3 cmHg
        and 23.2 cmHg, respectively. */
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=VDG;
 INST-ACC=2JPNKYU;
 INC-ENGY-LAB=[1.96MEV'4';
 /* '4' considering the energy loss of 190 keV in the nickel foil
        (1.6mg/cm**2 thick) at the entrance of target chamber and that
        of 320 keV in target gas */
 BEAM-INTNSTY=1UA'5';
 /* '5' average value */
 POL-PRJ=0%;
 DET-PARTCL=N;
 COINC=NO;
 ANT-COINC=NO;
 DET-SYS=PLATE'6';
 /* '6' Sakura NR-MI nuclear plates, 200 micron emulsion thickness
        used to detect neutrons */
 /* 2006-10-05 : Altered, Is. Re-digitized */
 RCT=14N(D,N)15O;
 PHQ=ANGL-DSTRN;
 MONTR-RCT=/ 2H(D,N)3HE /;
 ANL=X'9';
 /* '9' Stripping theory [A.B.Bhatia et al., Phil. Mag.
        43(1952)485] */
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,2;
 INC-ENGY-LAB=[1.96MEV'7';
 /* '7' considering the energy loss of 190 keV in the nickel foil
        (1.6mg/cm**2 thick) at the entrance of target chamber and that
        of 320 keV in target gas */
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 THTC DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA'10'
 (DEG) (MB/SR) (MB/SR)
 4.971E-01 2.396E+00 +-3.197E-01
 1.602E+01 3.080E+00 +-3.394E-01
 3.241E+01 3.764E+00 +-4.193E-01
 4.691E+01 2.490E+00 +-2.396E-01
 6.253E+01 2.455E+00 +-2.995E-01
 7.824E+01 1.861E+00 +-2.596E-01
 9.349E+01 1.406E+00 +-1.997E-01
 1.078E+02 1.511E+00 +-1.997E-01
 1.220E+02 2.593E+00 +-3.195E-01
 1.368E+02 4.874E+00 +-4.593E-01
 1.515E+02 7.973E+00 +-6.389E-01
 1.651E+02 1.045E+01 +-7.387E-01
 \END;
 /*===================================================================*/