266 research outputs found

    The functional model for maximal dissipative operators (translation form): An approach in the spirit of operator knots

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    In this article we develop a functional model for a general maximal dissipative operator. We construct the selfadjoint dilation of such operators. Unlike previous functional models, our model is given explicitly in terms of parameters of the original operator, making it more useful in concrete applications. For our construction we introduce an abstract framework for working with a maximal dissipative operator and its anti-dissipative adjoint and make use of the ˇStraus characteristic function in our setting. Explicit formulae are given for the selfadjoint dilation, its resolvent, a core and the completely non-selfadjoint subspace; minimality of the dilation is shown. The abstract theory is illustrated by the example of a Schrödinger operator on a half-line with dissipative potential, and boundary condition and connections to existing theory are discussed

    Boundary triplets and M-functions for non-selfadjoint operators, with applications to elliptic PDEs and block operator matrices

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    Starting with an adjoint pair of operators, under suitable abstract versions of standard PDE hypotheses, we consider the Weyl M-function of extensions of the operators. The extensions are determined by abstract boundary conditions and we establish results on the relationship between the M-function as an analytic function of a spectral parameter and the spectrum of the extension. We also give an example where the M-function does not contain the whole spectral information of the resolvent, and show that the results can be applied to elliptic PDEs where the M-function corresponds to the Dirichlet to Neumann map

    Conditions for the spectrum associated with a leaky wire to contain the interval [− α2/4, ∞)

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    The method of singular sequences is used to provide a simple and, in some respects, a more general proof of a known spectral result for leaky wires. The method introduces a new concept of asymptotic straightness

    Ends and means: experts debate the democratic oversight of the UK’s intelligence services

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    Revelations from Edward Snowden about the scope of intelligence activities in the UK have led to renewed attempts to enhance democratic oversight of the UK’s security services. The heads of MI5, MI6 and GCHQ appeared before the Intelligence and Security Committee for the first time, while Lord Macdonald called for strengthened parliamentary accountability. In this post, we ask democracy and security experts to consider the need for further reform

    Inverse problems for boundary triples with applications

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    This paper discusses the inverse problem of how much information on an operator can be determined/detected from `measurements on the boundary'. Our focus is on non-selfadjoint operators and their detectable subspaces (these determine the part of the operator `visible' from `boundary measurements'). We show results in an abstract setting, where we consider the relation between the M-function (the abstract Dirichlet to Neumann map or the transfer matrix in system theory) and the resolvent bordered by projections onto the detectable subspaces. More specifically, we investigate questions of unique determination, reconstruction, analytic continuation and jumps across the essential spectrum. The abstract results are illustrated by examples of Schr?odinger operators, matrix differential operators and, mostly, by multiplication operators perturbed by integral operators(the Friedrichs model), where we use a result of Widom to show that the detectable subspace can be characterized in terms of an eigenspace of a Hankel-like operator

    Weyl Solutions and jj-selfadjointness for Dirac Operators

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    We consider a non-selfadjoint Dirac-type differential expression (0.1)D(Q)y:=Jndydx+Q(x)y(0.1)D(Q)y := J_n {dy \over dx} +Q(x)y with a non-selfadjoint potential matrix QQ Ï”\epsilon LL ^{1}_{loc}(\scr J, \Bbb C^{n \times n}) and a signature matrix Jn=−Jn−J=−Jn∗J_n=-J^{-J}_n=-J^*_n Ï”\epsilon Cn×n\Bbb C ^{n \times n}. Here \scr J denotes either the line R\Bbb R or the half-line R+\Bbb R_+. With this differential expression one associates in L^2(\scr J, \Bbb C^n) the (closed) maximal and minimal operators Dmax(Q)D_{max}(Q) and Dmin(Q)D_{min}(Q), respectively. One of our main results for the whole line case states that Dmax(Q)=Dmin(Q)D_{max}(Q)=D_{min}(Q) in L2L^2 R,Cn\Bbb R, \Bbb C^n. Moreover, we show that if the minimal operator Dmin(Q)D_{min}(Q) in L2(R,Cn)L^2(\Bbb R, \Bbb C^n) is jj-symmetric with respect to an appropriate involution jj, then it is jj-selfadjoint. Similar results are valid in the case of the semiaxis R+\Bbb R_+. In particular, we show that if n=2pn=2p and the minimal operator Dmin+(Q)D^+_{min}(Q) in L2(R+,C2p)L^2(\Bbb R_+,\Bbb C^{2p}) is (\j\)-symmetric, then there exists a 2p×p−2p \times p-Weyl-type matrix solution. Κ(z,⋅)\Psi(z,\cdot) Ï”\epsilon L2(R+,C2p×p)L^2(\Bbb R_+, \Bbb C^{2p \times p}) of the equation Dmax+(Q)Κ(z,⋅)=zΚ(z,⋅)D^+_{max}(Q)\Psi(z,\cdot)=z \Psi(z,\cdot). A similar result is valid for the expression (0.1) whenever there exists a proper extension A~\tilde A with dim (dom A~\tilde A/dom Dmin+(Q))=pD^+_{min}(Q))=p and nonempty resolvent set. In particular, it holds if a potential matrix (\Q\) has a bounded imaginary part. This leads to the existence of a unique Weyl function for the express (0.1). The main results are proven by means of a reduction to the self-adjoint case by using the technique of dual pairs of operators. The differential expression (0.1) is of significance as it appears in the Lax formulation of the vector valued nonlinear Schrödinger equation

    The inverse problem for a spectral asymmetry function of the Schrodinger operator on a finite interval

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    For the Schroedinger equation −d2u/dx2+q(x)u=λu−d^2u/dx^2 + q(x)u = λu on a finite xx-interval, there is defined an “asymmetry function” a(λ;q)a(λ; q), which is entire of order 1/2 and type 1 in λλ. Our main result identifies the classes of square-integrable potentials q(x)q(x) that possess a common asymmetry function a(λ)a(λ). For any given a(λ)a(λ), there is one potential for each Dirichlet spectral sequence

    Essential Spectrum for Maxwell’s Equations

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    We study the essential spectrum of operator pencils associated with anisotropic Maxwell equations, with permittivity Δ, permeability ÎŒ and conductivity σ, on finitely connected unbounded domains. The main result is that the essential spectrum of the Maxwell pencil is the union of two sets: namely, the spectrum of the pencil div((ωΔ+iσ)∇⋅), and the essential spectrum of the Maxwell pencil with constant coefficients. We expect the analysis to be of more general interest and to open avenues to investigation of other questions concerning Maxwell’s and related systems
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