We address the decay rates of the energy for the damped wave equation when the damping
coefficient
does not satisfy the geometric control condition (GCC). First, we give a link
with the controllability of the associated Schrödinger equation. We prove
in an abstract setting that the observability of the Schrödinger equation
implies that the solutions of the damped wave equation decay at least like
(which is a stronger rate than the general logarithmic one predicted by the Lebeau
theorem).
Second, we focus on the 2-dimensional torus. We prove that the best decay one can
expect is
,
as soon as the damping region does not satisfy GCC. Conversely, for smooth damping
coefficients
vanishing flatly enough, we show that the semigroup decays at least like
, for
all
.
The proof relies on a second microlocalization around trapped directions, and
resolvent estimates.
In the case where the damping coefficient is a characteristic function of a strip (hence
discontinuous), Stéphane Nonnenmacher computes in an appendix part of the spectrum
of the associated damped wave operator, proving that the semigroup cannot decay faster
than
.
In particular, our study emphasizes that the decay rate highly depends on the way
vanishes.
Keywords
damped wave equation, polynomial decay, observability,
Schrödinger group, torus, two-microlocal semiclassical
measures, spectrum of the damped wave operator.