|
| /*===================================================================*/
/* NRDF D1870 Data No.3 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,3;
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,3;
/* 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 */
RCT=14N(D,N)15O;
PHQ=ANGL-DSTRN;
MONTR-RCT=/ 2H(D,N)3HE /;
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,3;
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'11'
(DEG) (MB/SR) (MB/SR)
0. 2.4 +-0.7
\END;
/*===================================================================*/
|