The energies and intensities of 58 gamma rays emitted in thermal-neutr
on capture by nitrogen (99.63% N-14) have been measured accurately. A
major reason was to establish this reaction as a standard for similar
measurements on other nuclides. These gamma rays have been placed betw
een 19 known levels (including the ground state and the capturing stat
e) in N-15. The primary gamma rays of both electric dipole (E1) and ma
gnetic dipole (M1) types have been analyzed with existing theories of
slow-neutron capture. Unlike many other light nuclides, the cross sect
ions for E1 transitions in N-15 differ drastically from the calculatio
ns of pure direct-capture theory. The role of the resonance-capture co
ntribution from the proton-unbound, neutron-bound level at 29+/-2 keV
below the neutron separation energy was considered. Some of the proper
ties of this level are quite well known from the C-14(p, gamma) reacti
on, and others can be derived from an R-matrix analysis of the total c
ross section as a function of neutron energy. The thermal-neutron capt
ure gamma-ray spectrum is different from the proton-capture gamma-ray
spectrum, but if proper account is taken of the interference among the
compound-nuclear processes, the valence-neutron mechanism, and potent
ial capture, the data can be satisfactorily explained. In the thermal-
neutron reaction, compound-nuclear E1 and direct-capture E1 contributi
ons are of comparable magnitude. Valence-neutron capture forms a signi
ficant component of capture by the neutron-bound level at -29 keV. Lar
gely destructive interference between compound-nuclear and valence pro
cesses in a few transitions in thermal-neutron capture gives rise to a
much smaller total cross section than would be obtained from the comp
ound-nuclear process alone. The M1 transitions also show some evidence
of a direct process but not a dominant one. The magnitudes of the com
pound-nuclear transitions, both E1 and M1, are largely consistent with
the values implied by giant resonance theories. The resonance paramet
ers deduced for the -29-keV level are: total radiation width=565+/-24
meV, reduced neutron width=51.6+/-0.3 keV (for a channel radius of 3.5
fm), and proton width=160+/-30 meV.