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PreprintCC BY 4.0arXiv

Extended stability timescales for the 2D3C rotating stratified Boussinesq equations

Abstract

We study the time evolution of a vertical-slice model for incompressible inhomogeneous rotating fluids perturbed around a stably stratified rest state with linear buoyancy profile. For ε-small localized initial data with vanishing potential vorticity, we prove that solutions remain of size O(ε) up to times of order ε−4/3, and up to times of order ε−2 in a regime where the Brunt--Väisälä frequency and the Coriolis parameter are comparable. The first result relies on linear dispersion with amplitude decay rate ⟨ t⟩−1/2, while the second exploits the absence of three-wave resonances via a normal form transformation. Our results remain valid for small nonzero initial potential vorticity, whose size is propagated by means of an intrinsic change of coordinates.

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BibTeX
@misc{zotto2026extended,
  title = {{Extended stability timescales for the 2D3C rotating stratified Boussinesq equations}},
  author = {Augusto Del Zotto and Luca Melzi and Haoling Xiang},
  howpublished = {arXiv},
  year = {2026},
  month = oct,
  doi = {10.48550/arxiv.2610.37013},
  eprint = {2610.37013},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2610.37013},
  note = {CC BY 4.0},
}
RIS
TY  - UNPB
TI  - Extended stability timescales for the 2D3C rotating stratified Boussinesq equations
AU  - Augusto Del Zotto
AU  - Luca Melzi
AU  - Haoling Xiang
PY  - 2026
DA  - 2026/10/27
PB  - arXiv
DO  - 10.48550/arxiv.2610.37013
UR  - https://arxiv.org/abs/2610.37013
AB  - We study the time evolution of a vertical-slice model for incompressible inhomogeneous rotating fluids perturbed around a stably stratified rest state with linear buoyancy profile. For ε-small localized initial data with vanishing potential vorticity, we prove that solutions remain of size O(ε) up to times of order ε^−4/3, and up to times of order ε^−2 in a regime where the Brunt--Väisälä frequency and the Coriolis parameter are comparable. The first result relies on linear dispersion with amplitude decay rate ⟨ t⟩^−1/2, while the second exploits the absence of three-wave resonances via a normal form transformation. Our results remain valid for small nonzero initial potential vorticity, whose size is propagated by means of an intrinsic change of coordinates.
ER  -