Abstract

Let (M, g) be a compact, smooth Riemannian manifold and $$\{u_h\}$$ be a sequence of $$L^2$$ -normalized Laplace eigenfunctions that has a localized defect measure $$\mu $$ in the sense that $$ M {\setminus } {{\text {supp}}}\!(\pi _* \mu ) \ne \emptyset $$ where $$\pi :T^*M \rightarrow M$$ is the canonical projection. Using Carleman estimates we prove that for any real smooth closed hypersurface $$H \subset (M{\setminus } {{\text {supp}}}\!(\pi _* \mu ))$$ sufficienly close to $$\text {supp} \, \pi _* \mu $$ and for all $$\delta >0,$$ $$\begin{aligned} \int _{H} |u_h|^2 d\sigma _{_{\!H}} \ge C_{\delta } e^{- [ \, {\varphi (\tau _{_{\!H}})} + \delta \, ] /h}, \end{aligned}$$ as $$h \rightarrow 0^+.$$ Here, $$\varphi (\tau ) = \tau + O(\tau ^2)$$ and $$\tau _{_{\!H}}:= d(H, {{\text {supp}}}\!(\pi _* \mu ))$$ . We also show that an analogous result holds for eigenfunctions of Schrödinger operators and give applications to eigenfunctions on warped products and joint eigenfunctions of quantum completely integrable (QCI) systems.

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.