2016
DOI: 10.2422/2036-2145.201409_005
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Sub-Laplacian eigenvalue bounds on sub-Riemannian manifolds

Abstract: We study eigenvalue problems for intrinsic sub-Laplacians on regular sub-Riemannian manifolds. We prove upper bounds for sub-Laplacian eigenvalues λ k of conformal sub-Riemannian metrics that are asymptotically sharp as k → +∞. For Sasakian manifolds with a lower Ricci curvature bound, and more generally, for contact metric manifolds conformal to such Sasakian manifolds, we obtain eigenvalue inequalities that can be viewed as versions of the classical results by Korevaar and Buser in Riemannian geometry.

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Cited by 26 publications
(25 citation statements)
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“…The key ingredient is a construction of disjoint sets whose measure is carefully controlled by our geometric hypotheses. Though similar ideas, originating in the work by Buser [8] and Korevaar [23], have been used in a few papers recently, see for example [21,24,22], and [25], our hypotheses are rather different from the previous work. In particular, we do not use a lower Ricci curvature bound for a background or auxiliary metric, which is so essential in most of the past papers.…”
Section: Introductionmentioning
confidence: 87%
“…The key ingredient is a construction of disjoint sets whose measure is carefully controlled by our geometric hypotheses. Though similar ideas, originating in the work by Buser [8] and Korevaar [23], have been used in a few papers recently, see for example [21,24,22], and [25], our hypotheses are rather different from the previous work. In particular, we do not use a lower Ricci curvature bound for a background or auxiliary metric, which is so essential in most of the past papers.…”
Section: Introductionmentioning
confidence: 87%
“…The difficulty compared from the 2-step case is the non-equality between y({X ni }) and Y ({X ni }). We will compute its difference by using the BCH formula (7).…”
Section: Higher Step Casesmentioning
confidence: 99%
“…Define the map P l : g → V l to be the linear projection. Then by the BCH formula (7), P l (y({X ni })) = 0 for l ≤ j − 1, P j (y({X ni })) = Y ({X ni }) = Z j , and P j (y({X ni })) does not vanish for i ≥ l + 1. We label the error term as follows.…”
Section: Higher Step Casesmentioning
confidence: 99%
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“…Laplace eigenvalue problem has the characteristics of strong practicability, continuable extension, and relatively complete theoretical system. This problem usually applied to particle motion, thermal magnetic radiation, lattice vibration [1], light thin film vibvicvib ration, graph theory [2], and Riemann manifolds theory [3].…”
Section: Introductionmentioning
confidence: 99%