Many diode laser structures, including those based on group-III nitride sys
tem, contain passive waveguide layers of higher refractive index than in th
e adjacent layers. Modes of such passive waveguides ("passive" modes) can i
nteract with an active layer mode ("active" mode), giving rise to two kinds
of normal modes or "supermodes" of a laser structure. Away from resonance,
one of them is localized predominantly in the active region ("lasing" mode
), while the other ones are located mostly in passive waveguides ("ghost" m
odes). The lasing mode is the mode at which laser generation occurs. The lo
ssy ghost modes are parasitic modes of a laser structure that can consume e
nergy from the active region. Resonant coupling occurs when the lasing mode
and a ghost mode are in phase synchronism. In this paper, the concept of g
host modes is applied to InGaN-based diode lasers, The values for critical
thickness are calculated for p-GaN cap layer and for n-GaN buffer/substrate
layer for a particular multilayer laser structure. The typical thickness o
f 0.5 mu m of AlGaN-cladding layer is found to be insufficient to prevent r
ather strong coupling between the modes, Under the resonant coupling condit
ions, the modal gain is shown to be strongly suppressed, allowing no lasing
at all.