It is commonly held that a necessary condition for the existence of soliton
s in nonlinear-wave systems is that the soliton's frequency (spatial or tem
poral) must not fall into the continuous spectrum of radiation modes. Howev
er, this is not always true. We present a new class of codimension-one soli
tons (i.e., those existing at isolated frequency values) that are embedded
into the continuous spectrum. This is possible if the spectrum of the linea
rized system has (at least) two branches, one corresponding to exponentiall
y localized solutions, and the other to radiation modes. An embedded solito
n (ES) is obtained when the latter component exactly vanishes in the solita
ry-wave's tail. The paper contains both a survey of recent results obtained
by the authors and some new results, the aim being to draw together severa
l different mechanism underlying the existence of ESs. We also consider the
distinctive properties of semi-stability of ESs, and moving ESs. Results a
re presented for four different physical models, including an extended fift
h-order KdV equation describing surface waves in inviscid fluids, and three
models from nonlinear optics. One of them pertains to a resonant Bragg gra
ting in an optical fiber with a cubic nonlinearity, while two others descri
be second-harmonic generation (SHG) in the temporal or spatial domain (i.e.
, respectively, propagating pulses in nonlinear-optical fibers, or stationa
ry patterns in nonlinear planar waveguides). Special attention is paid to t
he SHG model in the temporal domain for a case of competing quadratic and c
ubic nonlinearities. In particular, a new result is that when both harmonic
s have anomalous dispersion, an ES can exist which is, virtually, completel
y stable. (C) 2001 Elsevier Science B.V. All rights reserved.