2018
DOI: 10.1090/proc/14028
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A note on constructing families of sharp examples for 𝐿^{𝑝} growth of eigenfunctions and quasimodes

Abstract: In this note we analyse L p estimates for Laplacian eigenfunctions and quasimodes and their associated sharp examples. In particular we use previously determined estimates to produce a new set of estimates for restriction to thickened neighbourhoods of submanifolds. In addition we produce a family flat model quasimode examples that can be used to determine sharpness of estimates on Laplacian eigenfunctions restricted to subsets. For each quasimode in the family we show that there is a corresponding spherical h… Show more

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Cited by 8 publications
(2 citation statements)
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“…Note that in this paper we study averages of relatively weak quasimodes for the Laplacian with no additional assumptions on the functions. This is in contrast with results which impose additional conditions on the functions such as: that they be Laplace eigenfunctions that simultaneously satisfy additional equations [IS95, GT18b,Tac18]; that they be eigenfunctions in the very rigid case of the flat torus [Bou93,Gro85]; or that they form a density one subsequence of Laplace eigenfunctions [JZ16].…”
Section: Family Of Submanifolds Of Codimension K Satisfying (25)mentioning
confidence: 88%
“…Note that in this paper we study averages of relatively weak quasimodes for the Laplacian with no additional assumptions on the functions. This is in contrast with results which impose additional conditions on the functions such as: that they be Laplace eigenfunctions that simultaneously satisfy additional equations [IS95, GT18b,Tac18]; that they be eigenfunctions in the very rigid case of the flat torus [Bou93,Gro85]; or that they form a density one subsequence of Laplace eigenfunctions [JZ16].…”
Section: Family Of Submanifolds Of Codimension K Satisfying (25)mentioning
confidence: 88%
“…However, by carefully splitting into oscillatory regions where stationary phase can be applied and θ-dependent non-oscillatory regions similar to (1.12), it can be seen that at p = p c , f λ,θ L pc λ 1/pc for any θ ∈ [λ −1/2 , 1], hence its designation as the "critical" exponent. These computations were carried out rigorously in [Tac18].…”
Section: Introductionmentioning
confidence: 99%