Endpoint Mapping Properties of Wave Operators for Two-Dimensional Schrödinger Operators
Abstract
We establish sharp endpoint mapping properties for the wave operators W±(H,−Δ) of two-dimensional Schrödinger operators H=−Δ+V with real-valued decaying potentials V. Together with the known non-endpoint Lp theory, our results give a complete classification of the Lp mapping properties of the two-dimensional wave operators, and reveal an unexpected reversal of the usual threshold paradigm at the endpoints p=1 and p=∞. When zero is a regular point of H, the wave operators fail to be bounded on L1(ℝ2) and on L∞(ℝ2), but they satisfy the atural substitute estimates of Calderón--Zygmund type: L1(ℝ2)⟶ L1,∞(ℝ2), ℋ1(ℝ2)⟶ L1(ℝ2), L∞(ℝ2)⟶ BMO(ℝ2). When zero is instead a threshold singularity of the first kind---an s-wave resonance with no other threshold obstruction, the wave operators are bounded on both endpoint spaces L1(ℝ2) and L∞(ℝ2). Thus, in dimension two, an s-wave resonance improves the endpoint behavior of the wave operators, in sharp contrast with dimensions n≥3, where the only regular case is the favorable one. We also determine the endpoint behavior in the remaining zero-energy spectral configurations of H. A p-wave resonance obstructs both the L1- and the L∞-boundedness of the wave operators, while in the zero-eigenvalue case we obtain necessary and sufficient conditions for endpoint boundedness, expressed in terms of the presence of s- and p-wave resonances and of explicit second-order harmonic moment cancellations satisfied by the zero-energy eigenfunctions.
Related
- Endpoint Mapping Properties of Wave Operators for Schrödinger Operators in Dimensions n≥3
- Spectral-Edge Continuation, Dimensional Crossover, and Endpoint Stability for Partially Confined Nonlinear Schrödinger Equations
- Optimal bounds for embedded eigenvalues of one-dimensional discrete Schrödinger operators with decaying potentials
- Poisson statistics for one-dimensional Anderson--Bernoulli Schrödinger operators
- Lp-Liouville properties and realizations of Schrödinger operators on incomplete Riemannian manifolds
BibTeX
@misc{cheng2026endpoint,
title = {{Endpoint Mapping Properties of Wave Operators for Two-Dimensional Schrödinger Operators}},
author = {Han Cheng and Changxing Miao and Xiaohua Yao},
howpublished = {arXiv},
year = {2026},
month = sep,
doi = {10.48550/arxiv.2608.30602},
eprint = {2608.30602},
archivePrefix = {arXiv},
url = {https://arxiv.org/abs/2608.30602},
note = {CC BY 4.0},
}
RIS
TY - UNPB
TI - Endpoint Mapping Properties of Wave Operators for Two-Dimensional Schrödinger Operators
AU - Han Cheng
AU - Changxing Miao
AU - Xiaohua Yao
PY - 2026
DA - 2026/09/12
PB - arXiv
DO - 10.48550/arxiv.2608.30602
UR - https://arxiv.org/abs/2608.30602
AB - We establish sharp endpoint mapping properties for the wave operators W_±(H,−Δ) of two-dimensional Schrödinger operators H=−Δ+V with real-valued decaying potentials V. Together with the known non-endpoint L^p theory, our results give a complete classification of the L^p mapping properties of the two-dimensional wave operators, and reveal an unexpected reversal of the usual threshold paradigm at the endpoints p=1 and p=∞. When zero is a regular point of H, the wave operators fail to be bounded on L^1(ℝ^2) and on L^∞(ℝ^2), but they satisfy the atural substitute estimates of Calderón--Zygmund type: L^1(ℝ^2)⟶ L^1,∞(ℝ^2), ℋ^1(ℝ^2)⟶ L^1(ℝ^2), L^∞(ℝ^2)⟶ BMO(ℝ^2). When zero is instead a threshold singularity of the first kind---an s-wave resonance with no other threshold obstruction, the wave operators are bounded on both endpoint spaces L^1(ℝ^2) and L^∞(ℝ^2). Thus, in dimension two, an s-wave resonance improves the endpoint behavior of the wave operators, in sharp contrast with dimensions n≥3, where the only regular case is the favorable one. We also determine the endpoint behavior in the remaining zero-energy spectral configurations of H. A p-wave resonance obstructs both the L^1- and the L^∞-boundedness of the wave operators, while in the zero-eigenvalue case we obtain necessary and sufficient conditions for endpoint boundedness, expressed in terms of the presence of s- and p-wave resonances and of explicit second-order harmonic moment cancellations satisfied by the zero-energy eigenfunctions.
ER -