Generalized PT-symmetric operators acting an a Hilbert space $\mathfrak{H}$
are defined and investigated. The case of PT-symmetric extensions of a
symmetric operator $S$ is investigated in detail. The possible application of
the Lax-Phillips scattering methods to the investigation of PT-symmetric
operators is illustrated by considering the case of 0-perturbed operators.
We analyze the asymptotic behaviour of the heat kernel defined by a
stochastically perturbed geodesic flow on the cotangent bundle of a Riemannian
manifold for small time and small diffusion parameter. This extends WKB-type
methods to a particular case of a degenerate Hamiltonian. We derive uniform
bounds for the solution of the degenerate Hamiltonian boundary value problem
for small time. From this equivalence of solutions of the Hamiltonian equations
and the corresponding Hamilton Jacobi equation follows.
We prove the strong Feller property and ergodicity for 3D stochastic
Navier-Stokes equation driven by mildly degenerate noises (i.e. all but
finitely many Fourier modes are forced) via Galerkin approximation approach.
Given a self-adjoint involution J on a Hilbert space H, we consider a
J-self-adjoint operator L=A+V on H where A is a possibly unbounded self-adjoint
operator commuting with J and V a bounded J-self-adjoint operator
anti-commuting with J. We establish optimal estimates on the position of the
spectrum of L with respect to the spectrum of A and we obtain norm bounds on
the operator angles between maximal uniformly definite reducing subspaces of
the unperturbed operator A and the perturbed operator L.
Given a self-adjoint involution J on a Hilbert space H, we consider a
J-self-adjoint operator L=A+V on H where A is a possibly unbounded self-adjoint
operator commuting with J and V a bounded J-self-adjoint operator
anti-commuting with J. We establish optimal estimates on the position of the
spectrum of L with respect to the spectrum of A and we obtain norm bounds on
the operator angles between maximal uniformly definite reducing subspaces of
the unperturbed operator A and the perturbed operator L.
Using a method of stochastic perturbation of a Langevin system associated
with the non-viscous Burgers equation we construct a solution to the Riemann
problem for the pressureless gas dynamics describing sticky particles dynamics.
As a bridging step we consider a medium consisting of noninteracting particles.
We analyze the difference in the behavior of discontinuous solutions for these
two models and the relations between them. In our framework in 1D case we
obtain a unique entropy solution to the Riemann problem.