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Schrödinger estimates with arbitrarily small periodic regularity on ℍ2 × 𝕋

Abstract

Let M=ℍ2×𝕋 carry its product metric. We prove that the Schrödinger evolution maps L2(ℍ2;Hs(𝕋)) into L2([0,1];L6(M)) for every s>0, without any regularity assumption in the hyperbolic variable. The proof separates hyperbolic and periodic frequencies. A localized hyperbolic kernel estimate restricts the effective interaction time at hyperbolic frequency L to order L−1. Quadratic exponential sums then give a logarithmic bound when the periodic bandwidth is comparable to L. A mixed-norm decoupling argument, including an L6-valued extension and a periodic transference step, reduces wider periodic bands to this case. The infimum of the admissible periodic regularities is therefore zero. The estimate at zero regularity is not established here.

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BibTeX
@misc{wei2026schrödinger,
  title = {{Schrödinger estimates with arbitrarily small periodic regularity on $\mathbbH^2 \times \mathbbT$}},
  author = {Xuyi Wei},
  howpublished = {arXiv},
  year = {2026},
  month = oct,
  doi = {10.48550/arxiv.2610.27920},
  eprint = {2610.27920},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2610.27920},
}
RIS
TY  - UNPB
TI  - Schrödinger estimates with arbitrarily small periodic regularity on ℍ^2 × 𝕋
AU  - Xuyi Wei
PY  - 2026
DA  - 2026/10/20
PB  - arXiv
DO  - 10.48550/arxiv.2610.27920
UR  - https://arxiv.org/abs/2610.27920
AB  - Let M=ℍ^2×𝕋 carry its product metric. We prove that the Schrödinger evolution maps L^2(ℍ^2;H^s(𝕋)) into L^2([0,1];L^6(M)) for every s>0, without any regularity assumption in the hyperbolic variable. The proof separates hyperbolic and periodic frequencies. A localized hyperbolic kernel estimate restricts the effective interaction time at hyperbolic frequency L to order L^−1. Quadratic exponential sums then give a logarithmic bound when the periodic bandwidth is comparable to L. A mixed-norm decoupling argument, including an L^6-valued extension and a periodic transference step, reduces wider periodic bands to this case. The infimum of the admissible periodic regularities is therefore zero. The estimate at zero regularity is not established here.
ER  -