2018
DOI: 10.1007/s11854-018-0043-x
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The Morse and Maslov indices for Schrödinger operators

Abstract: We study the spectrum of Schrödinger operators with matrix valued potentials utilizing tools from infinite dimensional symplectic geometry. Using the spaces of abstract boundary values, we derive relations between the Morse and Maslov indices for a family of operators on a Hilbert space obtained by perturbing a given self-adjoint operator by a smooth family of bounded self-adjoint operators. The abstract results are applied to the Schrödinger operators with quasi-periodic, Dirichlet and Neumann boundary condit… Show more

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Cited by 9 publications
(7 citation statements)
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References 38 publications
(35 reference statements)
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“…We answer this question in the positive by reformulating it in terms of Lagrangian geometry. It is well known that self-adjoint extensions of a symmetric operator with equal deficiency indices are in one-to-one correspondence with the Lagrangian planes in some symplectic Hilbert space [AS80,BF,KS99,Ha00,LS,LSS,McS]. The question of restricting self-adjoint vertex conditions from the original graph to its reduced versionwith some edges shrunk to zero -is reframed in terms of the so-called linear symplectic reduction (see, for example, [McS]) allowing us to show that (1.1)-(1.2) indeed define a valid self-adjoint limiting operator.…”
Section: Introductionmentioning
confidence: 99%
“…We answer this question in the positive by reformulating it in terms of Lagrangian geometry. It is well known that self-adjoint extensions of a symmetric operator with equal deficiency indices are in one-to-one correspondence with the Lagrangian planes in some symplectic Hilbert space [AS80,BF,KS99,Ha00,LS,LSS,McS]. The question of restricting self-adjoint vertex conditions from the original graph to its reduced versionwith some edges shrunk to zero -is reframed in terms of the so-called linear symplectic reduction (see, for example, [McS]) allowing us to show that (1.1)-(1.2) indeed define a valid self-adjoint limiting operator.…”
Section: Introductionmentioning
confidence: 99%
“…The relevant technical properties of the Maslov index are summarized in Appendix B of [10]; a more complete presentation can be found in [4] or [14]. Some applications of the Maslov index to boundary value problems for PDE can be found in [10,11,12,17,22,27].…”
Section: Introductionmentioning
confidence: 99%
“…β(s, t) = {z + J ⊞ A(s, t)z : z ∈ β(0, 0)} , where J ⊞ (x, φ, y, ψ) = (R −1 φ, −Rx, −R −1 ψ, Ry)andR : H 1/2 (Σ) → H −1/2 (Σ) ∼ = (H 1/2 (Σ)) *is the Riesz duality isomorphism (cf. equation(17) in[10]). It suffices to choose A(s, t)(x, 0, 0, ψ) = − R −1 (tψ + sJ x), 0, 0, tRx , which is selfadjoint because the composition R −1 • J :H 1/2 (Σ) → H 1/2 (Σ) is selfadjoint.To prove the selfadjointness of R −1 • J we use the identity R −1 = R * to computeR −1 J f, g H 1/2 (Σ) = J f, Rg H −1/2 (Σ) = (J f )g = Σ f g for any f, g ∈ H 1/2 (Σ),where (J f )g denotes the action of the functional J f ∈ H −1/2 (Σ) on g ∈ H 1/2 (Σ).…”
mentioning
confidence: 99%
“…In this section, we discuss an infinitesimal version of the formula equating the Maslov index and the spectral flow for the family of operators H t = A t + V t satisfying Hypothesis 4.3, which is assumed throughout this section. Formulas relating these two quantities are quite classical, and we refer the reader to the papers [19,20,21,22,26,35,36,48,71,72,73,88] and the literature therein. Employing the abstract Hadamard-type formula obtained in Theorem 3.23, we prove in Theorem 4.19 that the signature of the Maslov crossing form defined in (4.34) at an eigenvalue λ of the operator H t0 is equal to the difference between the number of monotonically decreasing and the number of monotonically increasing eigenvalue curves for H t bifurcating from λ.…”
Section: 4mentioning
confidence: 99%