Abstract
This article shows that for a large class of discrete periodic Schrödinger operators, most wavefunctions resemble Bloch states. More precisely, we prove quantum ergodicity for a family of periodic Schrödinger operators H on periodic graphs. This means that most eigenfunctions of H on large finite periodic graphs are equidistributed in some sense, hence delocalized. Our results cover the adjacency matrix on \(\mathbb {Z}^d\), the triangular lattice, the honeycomb lattice, Cartesian products, and periodic Schrödinger operators on \(\mathbb {Z}^d\). The theorem applies more generally to any periodic Schrödinger operator satisfying an assumption on the Floquet eigenvalues.
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Notes
It is worthwhile to note that in the case of trees [1, 3, 4], we usually evolve the dynamical system in time T, essentially up to the girth of the graph, take the size of the graph \(N\rightarrow \infty \), then finally take \(T\rightarrow \infty \). Here we first consider the equilibrium limit in T, then take \(N\rightarrow \infty \) in the end of the proof.
Note that we only discussed the (ir)-reducibility of the Bloch variety here. The irreducibility of the Fermi variety, where \(\lambda \) is fixed, is significantly harder to prove [22], but we do not need it.
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Communicated by J. Ding.
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T. McKenzie: Supported by NSF GRFP Grant DGE-1752814 and NSF Grant DMS-2212881.
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McKenzie, T., Sabri, M. Quantum Ergodicity for Periodic Graphs. Commun. Math. Phys. 403, 1477–1509 (2023). https://doi.org/10.1007/s00220-023-04826-2
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DOI: https://doi.org/10.1007/s00220-023-04826-2