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- Partial differential equations (4)
- dissipative Schroedinger-type operators (4)
- discontinuous coefficients (3)
- nonsmooth domains (3)
- Elliptic transmission problems (2)
- Lax-Phillips scattering theory (2)
- Sturm-Liouville operators (2)
- carrier and current densities (2)
- characteristic function (2)
- density matrices (2)
We prove an optimal regularity result for elliptic operators $-\nabla \cdot \mu \nabla:W^1,q_0 \rightarrow W^-1,q$ for a $q>3$ in the case when the coefficient function $\mu$ has a jump across a $C^1$ interface and is continuous elsewhere. A counterexample shows that the $C^1$ condition cannot be relaxed in general. Finally, we draw some conclusions for corresponding parabolic operators.
Let $\Upsilon$ be a three-dimensional Lipschitz polyhedron, and assume that the matrix function $\mu$ is piecewise constant on a polyhedral partition of $\Upsilon$. Based on regularity results for solutions to two-dimensional anisotropic transmission problems near corner points we obtain conditions on $\mu$ and the intersection angles between interfaces and $\partial \Upsilon$ ensuring that the operator $-\nabla \cdot \mu \nabla$ maps the Sobolev space $W^1,q_0(\Upsilon)$ isomorphically onto $W^-1,q(\Upsilon)$ for some $q > 3$.
Using a classical theorem of Sobolevskii on equations of parabolic type in a Banach space and recently obtained results on elliptic operators with discontinuous coefficients including mixed boundary conditions we prove that quasilinear parabolic systems in diagonal form admit a local, classical solution in the space of p-integrable functions, for some p greater than 1, over a bounded two dimensional space domain. As applications we have in mind systems of reaction diffusion equations, e.g. van Roosbroeck's system. The treatment of such equations in a space of integrable functions enables us to define the normal component of the flow across any part of the Dirichlet boundary by Gauss' theorem.
For an operator-valued block-matrix model, which is called in quantum physics a Feshbach decomposition, a scattering theory is considered. Under trace class perturbation the channel scattering matrices are calculated. Using Feshbach's optical potential it is shown that for a given spectral parameter the channel scattering matrices can be recovered either from a dissipative or from a Lax-Phillips scattering theory.
The paper is devoted to Schroedinger operators on bounded intervals of the real axis with dissipative boundary conditions. In the framework of the Lax-Phillips scattering theory the asymptotic behaviour of the phase shift is investigated in detail and its relation to the spectral shift is discussed, in particular, trace formula and Birman-Krein formula are verified directly. The results are used for dissipative Schroedinger-Poisson systems.
We describe an embedding of a quantum mechanically described structure into a macroscopic flow. The open quantum system is partly driven by an adjacent macroscopic flow acting on the boundary of the bounded spatial domain designated to quantum mechanics. This leads to an essentially non-selfadjoint Schroedinger-type operator, the spectral properties of which will be investigated.
We study in detail Schroedinger-type operators on a bounded interval of the real axis with dissipative boundary conditions. The characteristic function of such operators is computed, its minimal self-adjoint dilation is constructed and the generalized eigenfunction expansion for the dilation is developed. The problem is motivated by semiconductor physics.
A 1D coupled drift-diffusion dissipative Schroedinger model (hybrid model), which
is capable to describe the transport of electrons and holes in semi-conductor devices
in a non-equilibrium situation, is mathematically analyzed. The device domain is
split into a part where the transport is well-described by the drift-diffusion equations
(classical zone) and a part where a quantum description via a dissipative Schroedinger
system (quantum zone) is used. Both system are coupled such that the continuity
of the current densities is guaranteed. The electrostatic potential is self-consistently
determined by Poisson's equation on the whole device. We show that the hybrid
model is well-posed, prove existence of solutions and show their uniform boundedness
provided the distribution function satisfy a so-called balance condition. The current
densities are different from zero in the non-equilibrium case and uniformly bounded.
We study a stationary Schrödinger-Poisson system on a bounded interval of the real axis. The Schrödinger operator is defined on the bounded domain with transparent boundary conditions. This allows us to model a non-zero current through the boundary of the interval. We prove that the system always admits a solution and give explicit a priori estimates for the solutions.
Let H be a semi–bounded self–adjoint operator in a separable Hilbert space.
For a certain class of positive, continuous, decreasing, and convex functions
F we show the convexity of trace functionals tr(F (H + U − ε(U ))) − ε(U ),
where U is a bounded self–adjoint operator on H and ε(U ) is a normalizing
real function—the Fermi level—which may be identical zero. If additionally
F is continuously differentiable, then the corresponding trace functional is
Fréchet differentiable and there is an expression of its gradient in terms off
the derivative of F . The proof of the differentiability of the trace functional
is based upon Birman and Solomyak’s theory of double Stieltjes operator
integrals. If, in particular, H is a Schrödinger–type operator and U a real-valued function, then the gradient of the trace functional is the quantum
mechanical expression of the particle density with respect to an equilibrium
distribution function f = −F . Thus, the monotonicity of the particle density
in its dependence on the potential U of Schrödinger’s operator—which has
been understood since the late 1980s—follows as a special case.