Excitation of accelerating modes in transversely inhomogeneous plasma chann
els is considered as an initial value problem. Discrete eigenmodes are supp
orted by plasma channels with sharp density gradients. These eigenmodes are
collisionlessly damped as the gradients are smoothed. Using collisionless
Landau damping as the analogy, the existence and damping of these "quasi-mo
des" is studied by constructing and analytically continuing the causal Gree
n's function of wake excitation into the lower half of the complex frequenc
y plane. Electromagnetic nature of the plasma wakes in the channel makes th
eir excitation nonlocal. This results in the algebraic decay of the fields
with time due to phase-mixing of plasma oscillations with spatially-varying
frequencies. Characteristic decay rate is given by the mixing time tau(m),
which corresponds to the dephasing of two plasma fluid elements separated
by the collisionless skin depth. For wide channels analytic expressions for
the field evolution are derived. Implications for electron acceleration in
plasma channels are discussed. (C) 1999 American Institute of Physics. [S1
070-664X(99)00902-7].