2011
DOI: 10.2422/2036-2145.2011.3.07
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Markov uniqueness of degenerate elliptic operators

Abstract: Let be an open subset of R d and H = − d i, j=1 ∂ i c i j ∂ j be a second-order partial differential operator on L 2 ( ) with domain C ∞ c ( ), where the coefficients c i j ∈ W 1,∞ ( ) are real symmetric and C = (c i j ) is a strictly positive-definite matrix over . In particular, H is locally strongly elliptic. We analyze the submarkovian extensions of H , i.e., the self-adjoint extensions that generate submarkovian semigroups. Our main result states that H is Markov unique, i.e., it has a unique submarkovian… Show more

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Cited by 8 publications
(21 citation statements)
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References 26 publications
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“…By using the results contained in [23], [24] and [7], we expect that our results can be further generalized to hold on domains with a Lipschitz boundary. Lastly let us notice that the Fukushima-Watanabe theorem has been recently extended by Robinson and Sikora (see [45], Theorem 1.1) to the case of an elliptic operator on an arbitrary open bounded set Ω; the final goal should be to generalize the results here presented to the case of such sets, replacing the topological boundary with the Martin one. • Given an orthogonal projector Π : h → h, we use the same symbol Π to denote both the injection Π|R(Π) : R(Π) → h and the surjection (Π|R(Π)) * : h → R(Π); • E(h) denotes the set of couples (Π, Θ), where Π is an orthogonal projection in h and Θ is a self-adjoint operator in the Hilbert space R(Π);…”
Section: Introductionmentioning
confidence: 95%
“…By using the results contained in [23], [24] and [7], we expect that our results can be further generalized to hold on domains with a Lipschitz boundary. Lastly let us notice that the Fukushima-Watanabe theorem has been recently extended by Robinson and Sikora (see [45], Theorem 1.1) to the case of an elliptic operator on an arbitrary open bounded set Ω; the final goal should be to generalize the results here presented to the case of such sets, replacing the topological boundary with the Martin one. • Given an orthogonal projector Π : h → h, we use the same symbol Π to denote both the injection Π|R(Π) : R(Π) → h and the surjection (Π|R(Π)) * : h → R(Π); • E(h) denotes the set of couples (Π, Θ), where Π is an orthogonal projection in h and Θ is a self-adjoint operator in the Hilbert space R(Π);…”
Section: Introductionmentioning
confidence: 95%
“…. But this criterion is a boundary condition and in earlier papers [RS11a] [RS11b] [Rob13] it was established that it is equivalent to Γ having zero capacity relative to the form h 0 . These earlier results were stated for forms with coefficients c kl ∈ W 1,∞ (Ω) or W 1,∞ loc (Ω) but in fact no smoothness of the coefficients is necessary.…”
Section: Preliminariesmentioning
confidence: 99%
“…Then h N is a Dirichlet form and the associated operator H N is the extension of H 0 corresponding to generalized Neumann boundary conditions. But if k is a general Dirichlet form extension of h 0 then D(h D ) ⊆ D(k) ⊆ D(h N ) (see [FOT94], Section 3.3, [RS11a], Theorem 1.1, or [RS11b], Theorem 2.1). Thus h N ≤ k ≤ h D in the sense of ordering of quadratic forms.…”
Section: Introductionmentioning
confidence: 99%
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“…For divergence type forms without potential a characterization of E (N) = E (D) is given in [RS11] (also compare [GM13] for analog results on weighted manifolds) in terms of the capacity of the boundary: For a measurable set A ⊂ Ω the capacity is defined as This result has been generalized to more than one dimension and improved in various directions. We just mention as one example the conditions given in Thm.…”
Section: Proposition 423mentioning
confidence: 99%