Making use of detailed pointwise Green's function bounds obtained in a prev
ious work for the linearized equations about the wave, we give a straightfo
rward derivation of the (nonlinear) L-P-asymptotic behavior of;a scalar (pl
anar) viscous shock front under perturbations in L-1 boolean AND L-infinity
with first moment in the normal direction to the front, in all dimensions
d greater than or equal to 2. For dimension d greater than or equal to 3, w
e establish sharp LP decay rates by a much simpler argument using only L-P
information on the Green's function, for perturbations merely in L-1 boolea
n AND L-infinity. These results simplify and greatly extend previous result
s of Goodman-Miller and Goodman, respectively which were obtained under ass
umptions of weak shock strength and artificial (identity) viscosity, and, i
n the case of asymptotic behavior, exponential decay of perturbations in th
e direction normal to the shock front. For perturbations localized as (1+\x
(1)\)(-1) in the normal direction, but not possessing a first moment, we gi
ve a refined picture of the linearized L-P-asymptotic behavior different fr
om the near-field approximation of Goodman and Miller.