Considered as rest points of ODE on L-p, stationary viscous shock waves pre
sent a critical case for which standard semigroup methods do not suffice to
determine stability. More precisely, there is no spectral gap between stat
ionary modes and essential spectrum of the linearized operator about the wa
ve, a fact that precludes the usual analysis by decomposition into invarian
t subspaces. For this reason, there have been until recently no results on
shock stability from the semigroup perspective except in the scalar or tota
lly compressive case ([Sat], [K.2], resp.), each of which can be reduced to
the standard semigroup setting by Sattinger's method of weighted norms. We
overcome this difficulty in the general case by the introduction of new, p
ointwise semigroup techniques, generalizing earlier work of Howard [H.1], K
apitula [K.1-2], and Zeng [Ze,LZe]. These techniques allow us to do "hard"
analysis in PDE within the dynamical systems/semigroup framework: in partic
ular, to obtain sharp, global pointwise bounds on the Green's function of t
he linearized operator around the wave, sufficient for the analysis of line
ar and nonlinear stability. The method is general, and should find applicat
ions also in other situations of sensitive stability.
Central to our analysis is a notion of "effective" point spectrum that can
be extended to regions of essential spectrum. This turns out to be intimate
ly related to the Evans function, a well-known tool for the spectral analys
is of traveling waves. Indeed, crucial to our whole analysis is the "Gap Le
mma" of [GZ,KS], a technical result developed originally in the context of
Evans function theory. Using these new tools, we can treat general over- an
d undercompressive, and even strong shock waves for systems within the same
framework used for standard weak (i.e. slowly varying) Lax waves. In all c
ases, we show that stability is determined by the simple and numerically co
mputable condition that the number of zeroes of the Evans function in the r
ight complex halfplane be equal to the dimension of the stationary manifold
of nearby traveling wave solutions. Interpreting this criterion in the con
servation law setting, we quickly recover all known analytic stability resu
lts, obtaining several new results as well.