Abstract:It is well known that the sum of negative (positive) eigenvalues of some
finite Hermitian matrix $V$ is concave (convex) with respect to $V$. Using the
theory of the spectral shift function we generalize this property to
self-adjoint operators on a separable Hilbert space with an arbitrary spectrum.
More precisely, we prove that the spectral shift function integrated with
respect to the spectral parameter from $-\infty$ to $\lambda$ (from $\lambda$
to $+\infty$) is concave (convex) with respect to trace class … Show more
“…[59], and the study of surface potentials, see [10,36]. Various of its properties are discussed in the literature: monotonicity and concavity in [20,22,35], the asymptotic behaviour in the large coupling constant [43,46,44] and semiclassical limit [42,40]. See [5,34] for surveys.…”
Abstract. We study spectra of Schrödinger operators on R d . First we consider a pair of operators which differ by a compactly supported potential, as well as the corresponding semigroups. We prove almost exponential decay of the singular values µn of the difference of the semigroups as n → ∞ and deduce bounds on the spectral shift function of the pair of operators.Thereafter we consider alloy type random Schrödinger operators. The single site potential u is assumed to be non-negative and of compact support. The distributions of the random coupling constants are assumed to be Hölder continuous. Based on the estimates for the spectral shift function, we prove a Wegner estimate which implies Hölder continuity of the integrated density of states.
“…[59], and the study of surface potentials, see [10,36]. Various of its properties are discussed in the literature: monotonicity and concavity in [20,22,35], the asymptotic behaviour in the large coupling constant [43,46,44] and semiclassical limit [42,40]. See [5,34] for surveys.…”
Abstract. We study spectra of Schrödinger operators on R d . First we consider a pair of operators which differ by a compactly supported potential, as well as the corresponding semigroups. We prove almost exponential decay of the singular values µn of the difference of the semigroups as n → ∞ and deduce bounds on the spectral shift function of the pair of operators.Thereafter we consider alloy type random Schrödinger operators. The single site potential u is assumed to be non-negative and of compact support. The distributions of the random coupling constants are assumed to be Hölder continuous. Based on the estimates for the spectral shift function, we prove a Wegner estimate which implies Hölder continuity of the integrated density of states.
“…For many more references the interested reader can consult [23], [24], [26], [27], [58], [60]. For recent results we refer to [25], [35], [59], [61], [62], and [64].…”
Abstract. We obtain a new representation for the solution to the operator Sylvester equation in the form of a Stieltjes operator integral. We also formulate new sufficient conditions for the strong solvability of the operator Riccati equation that ensures the existence of reducing graph subspaces for block operator matrices. Next, we extend the concept of the Lifshits-Krein spectral shift function associated with a pair of self-adjoint operators to the case of pairs of admissible operators that are similar to self-adjoint operators. Based on this new concept we express the spectral shift function arising in a perturbation problem for block operator matrices in terms of the angular operators associated with the corresponding perturbed and unperturbed eigenspaces.
“…A detailed account on the theory of the spectral shift function can be found in the review [4] and in the book [25]. For recent studies we refer to [14,10] and references therein. Recently the spectral shift function found a number of applications in the theory of random Schrödinger operators [15], [16], [17], [5], [6], [23], [18], [8].…”
dedicated to jean michel combes on the occasion of his 60 th birthdayWe prove that the integrated surface density of states of continuous or discrete Anderson-type random Schrödinger operators is a measurable locally integrable function rather than a signed measure or a distribution. This generalizes our recent results on the existence of the integrated surface density of states in the continuous case and those of A. Chahrour in the discrete case. The proof uses the new L p -bound on the spectral shift function recently obtained by Combes, Hislop, and Nakamura. Also we provide a simple proof of their result on the Hölder continuity of the integrated density of bulk states.
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