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.
We prove a lower bound for the k-th Steklov eigenvalues in terms of an isoperimetric constant called the k-th Cheeger-Steklov constant in three different situations: finite spaces, measurable spaces, and Riemannian manifolds. These lower bounds can be considered as higher order Cheeger type inequalities for the Steklov eigenvalues. In particular it extends the Cheeger type inequality for the first nonzero Steklov eigenvalue previously studied by Escobar in 1997 and by Jammes in 2015 to higher order Steklov eigenvalues. The technique we develop to get this lower bound is based on considering a family of accelerated Markov operators in the finite and mesurable situations and of mass concentration deformations of the Laplace-Beltrami operator in the manifold setting which converges uniformly to the Steklov operator. As an intermediary step in the proof of the higher order Cheeger type inequality, we define the Dirichlet-Steklov connectivity spectrum and show that the Dirichlet connectivity spectra of this family of operators converges to (or is bounded by) the Dirichlet-Steklov spectrum uniformly. Moreover, we obtain bounds for the Steklov eigenvalues in terms of its Dirichlet-Steklov connectivity spectrum which is interesting in its own right and is more robust than the higher order Cheeger type inequalities. The Dirichlet-Steklov spectrum is closely related to the Cheeger-Steklov constants.
Given two compact Riemannian manifolds M 1 and M 2 such that their respective boundaries Σ 1 and Σ 2 admit neighbourhoods Ω 1 and Ω 2 which are isometric, we prove the existence of a constant C such that |σ k (M 1 ) − σ k (M 2 )| ≤ C for each k ∈ N. The constant C depends only on the geometry of Ω 1 ∼ = Ω 2 . This follows from a quantitative relationship between the Steklov eigenvalues σ k of a compact Riemannian manifold M and the eigenvalues λ k of the Laplacian on its boundary. Our main result states that the difference |σ k − √ λ k | is bounded above by a constant which depends on the geometry of M only in a neighbourhood of its boundary. The proofs are based on a Pohozaev identity and on comparison geometry for principal curvatures of parallel hypersurfaces. In several situations, the constant C is given explicitly in terms of bounds on the geometry of Ω 1 ∼ = Ω 2 .1991 Mathematics Subject Classification. 35P15 (primary), 58C40, 35P20 (secondary).1 The notation O(k −∞ ) designates a quantity which tends to zero faster than any power of k.
We obtain upper bounds for the eigenvalues of the Schr\"odinger operator
$L=\Delta_g+q$ depending on integral quantities of the potential $q$ and a
conformal invariant called the min-conformal volume. Moreover, when the
Schr\"odinger operator $L$ is positive, integral quantities of $q$ which appear
in upper bounds, can be replaced by the mean value of the potential $q$. The
upper bounds we obtain are compatible with the asymptotic behavior of the
eigenvalues. We also obtain upper bounds for the eigenvalues of the weighted
Laplacian or the Bakry-Emery Laplacian
$\Delta_\phi=\Delta_g+\nabla_g\phi\cdot\nabla_g$ using two approaches: First,
we use the fact that $\Delta_\phi$ is unitarily equivalent to a Schr\"odinger
operator and we get an upper bound in terms of the $L^2$-norm of $\nabla_g\phi$
and the min-conformal volume. Second, we use its variational characterization
and we obtain upper bounds in terms of the $L^\infty$-norm of $\nabla_g\phi$
and a new conformal invariant. The second approach leads to a Buser type upper
bound and also gives upper bounds which do not depend on $\phi$ when the
Bakry-Emery Ricci curvature is non-negative
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