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MATHEMATICS
On the spectrum of a two-dimensional generalized periodic Schrödinger operator. II
L. I. Danilov Physical Technical Institute, Ural Branch of the Russian Academy
of Sciences, ul. Kirova, 132, Izhevsk, 426000, Russia
Abstract:
The paper is concerned with the problem of absolute continuity of the spectrum of the two-dimensional generalized periodic Schrödinger operator
$H_g+V=-\nabla g\nabla +V$ where the continuous positive function
$g$ and the scalar potential
$V$ have a common period lattice
$\Lambda $. The solutions of the equation
$(H_g+V)\varphi =0$ determine, in particular, the electric field and the magnetic field of electromagnetic waves propagating in two-dimensional photonic crystals. The function
$g$ and the scalar potential
$V$ are expressed in terms of the electric permittivity
$\varepsilon $ and the magnetic permeability
$\mu $ (
$V$ also depends on the frequency of the electromagnetic wave). The electric permittivity
$\varepsilon $ may be a discontinuous function (and usually it is chosen to be piecewise constant) so the problem to relax the known smoothness conditions on the function
$g$ that provide absolute continuity of the spectrum of the operator
$H_g+V$ arises. In the present paper we assume that the Fourier coefficients of the functions
$g^{\pm \frac 12}$ for some
$q\in [1,\frac 43 )$ satisfy the condition $\sum \bigl( |N|^{\frac 12}|(g^{\pm \frac 12})_N|\bigr) ^q < +\infty $, and the scalar potential
$V$ has relative bound zero with respect to the operator
$-\Delta $ in the sense of quadratic forms. Let
$K$ be the fundamental domain of the lattice
$\Lambda $, and assume that
$K^*$ is the fundamental domain of the reciprocal lattice
$\Lambda ^*$. The operator
$H_g+V$ is unitarily equivalent to the direct integral of operators
$H_g(k)+V$, with quasimomenta
$k\in 2\pi K^*$, acting on the space
$L^2(K)$. The last operators can be also considered for complex vectors
$k+ik^{\prime }\in {\mathbb C}^2$. We use the Thomas method. The proof of absolute continuity of the spectrum of the operator
$H_g+V$ amounts to showing that the operators
$H_g(k+ik^{\prime })+V-\lambda $,
$\lambda \in {\mathbb R}$, are invertible for some appropriately chosen complex vectors
$k+ik^{\prime }\in {\mathbb C}^2$ (depending on
$g$,
$V$, and the number
$\lambda $) with sufficiently large imaginary parts
$k^{\prime }$.
Keywords:
generalized Schrödinger operator, absolute continuity of the spectrum, periodic potential.
UDC:
517.958+
517.984.5
MSC: 35P05 Received: 28.02.2014
DOI:
10.20537/vm140201