522 research outputs found

    A Jost-Pais-type reduction of (modified) Fredholm determinants for semi-separable operators in infinite dimensions

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    We study the analog of semi-separable integral kernels in H\mathcal{H} of the type K(x,xβ€²)={F1(x)G1(xβ€²),a<xβ€²<x<b,F2(x)G2(xβ€²),a<x<xβ€²<b, K(x,x')=\begin{cases} F_1(x)G_1(x'), & a<x'< x< b, \\ F_2(x)G_2(x'), & a<x<x'<b, \end{cases} where βˆ’βˆžβ‰€a<bβ‰€βˆž-\infty\leq a<b\leq \infty, and for a.e.\ x∈(a,b)x \in (a,b), Fj(x)∈B2(Hj,H)F_j (x) \in \mathcal{B}_2(\mathcal{H}_j,\mathcal{H}) and Gj(x)∈B2(H,Hj)G_j(x) \in \mathcal{B}_2(\mathcal{H},\mathcal{H}_j) such that Fj(β‹…)F_j(\cdot) and Gj(β‹…)G_j(\cdot) are uniformly measurable, and βˆ₯Fj(β‹…)βˆ₯B2(Hj,H)∈L2((a,b)),β€…β€Šβˆ₯Gj(β‹…)βˆ₯B2(H,Hj)∈L2((a,b)),j=1,2, \|F_j(\cdot)\|_{\mathcal{B}_2(\mathcal{H}_j,\mathcal{H})} \in L^2((a,b)), \; \|G_j (\cdot)\|_{\mathcal{B}_2(\mathcal{H},\mathcal{H}_j)} \in L^2((a,b)), \quad j=1,2, with H\mathcal{H} and Hj\mathcal{H}_j, j=1,2j=1,2, complex, separable Hilbert spaces. Assuming that K(β‹…,β‹…)K(\cdot, \cdot) generates a Hilbert-Schmidt operator K\mathbf{K} in L2((a,b);H)L^2((a,b);\mathcal{H}), we derive the analog of the Jost-Pais reduction theory that succeeds in proving that the modified Fredholm determinant det⁑2,L2((a,b);H)(Iβˆ’Ξ±K){\det}_{2, L^2((a,b);\mathcal{H})}(\mathbf{I} - \alpha \mathbf{K}), α∈C\alpha \in \mathbb{C}, naturally reduces to appropriate Fredholm determinants in the Hilbert spaces H\mathcal{H} (and HβŠ•H\mathcal{H} \oplus \mathcal{H}). Some applications to Schr\"odinger operators with operator-valued potentials are provided.Comment: 25 pages; typos removed. arXiv admin note: substantial text overlap with arXiv:1404.073

    Principal Solutions Revisited

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    The main objective of this paper is to identify principal solutions associated with Sturm-Liouville operators on arbitrary open intervals (a,b)βŠ†R(a,b) \subseteq \mathbb{R}, as introduced by Leighton and Morse in the scalar context in 1936 and by Hartman in the matrix-valued situation in 1957, with Weyl-Titchmarsh solutions, as long as the underlying Sturm-Liouville differential expression is nonoscillatory (resp., disconjugate or bounded from below near an endpoint) and in the limit point case at the endpoint in question. In addition, we derive an explicit formula for Weyl-Titchmarsh functions in this case (the latter appears to be new in the matrix-valued context).Comment: 27 pages, expanded Sect. 2, added reference

    On a problem in eigenvalue perturbation theory

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    We consider additive perturbations of the type Kt=K0+tWK_t=K_0+tW, t∈[0,1]t\in [0,1], where K0K_0 and WW are self-adjoint operators in a separable Hilbert space H\mathcal{H} and WW is bounded. In addition, we assume that the range of WW is a generating (i.e., cyclic) subspace for K0K_0. If Ξ»0\lambda_0 is an eigenvalue of K0K_0, then under the additional assumption that WW is nonnegative, the Lebesgue measure of the set of all t∈[0,1]t\in [0,1] for which Ξ»0\lambda_0 is an eigenvalue of KtK_t is known to be zero. We recall this result with its proof and show by explicit counterexample that the nonnegativity assumption Wβ‰₯0W\geq 0 cannot be removed.Comment: 10 pages; added Lemma 2.4, typos removed; to appear in J. Math. Anal. App
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