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PreprintCC BY 4.0arXiv

On space-time derivative estimates for the fractional Navier-Stokes equations

Abstract

In this paper, we are concerned with space-time derivative estimates of solutions to the fractional Navier-Stokes equations. It is shown that Λnαu(m)t ∈ L(2(6α−5))/(4mα+2nα+4 α−5) (0,T; L2(ℝ3)) and $ Λ^{n }u^{(m)}_{t} \in L^{\frac{2(6α-5)}{4mα+2n +4 α-5}}~~~~~(0,T; L^{2}(\mathbb{R}^{3}))$. This generalizes a priori bounds for the classical Navier-Stokes system by Duff in [7, Acta Math. 164, 1990] and Boutros and Gibbon's spatial derivative estimates in [1, Nonlinearity 37, 2024]. In addition, we derive that $ u \in L^{\frac{q}{q-3}}~~(0,T;L^{q} (\mathbb{R}^{3}))$ with $ 6\leq q\leq\infty $ and $Λ^{k}u \in L^{\frac{q}{ q(k+1)-3}}~~~(0,T;L^{q} (\mathbb{R}^{3})) $ with $k\geq1, 2\leq q\leq\infty $ in the standard Navier-Stokes equations.

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BibTeX
@misc{wang2026spacetime,
  title = {{On space-time derivative estimates for the fractional Navier-Stokes equations}},
  author = {Yanqing Wang and Wei Wei and Gang Wu and Daoguo Zhou},
  howpublished = {arXiv},
  year = {2026},
  month = sep,
  doi = {10.48550/arxiv.2609.12864},
  eprint = {2609.12864},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2609.12864},
  note = {CC BY 4.0},
}
RIS
TY  - UNPB
TI  - On space-time derivative estimates for the fractional Navier-Stokes equations
AU  - Yanqing Wang
AU  - Wei Wei
AU  - Gang Wu
AU  - Daoguo Zhou
PY  - 2026
DA  - 2026/09/11
PB  - arXiv
DO  - 10.48550/arxiv.2609.12864
UR  - https://arxiv.org/abs/2609.12864
AB  - In this paper, we are concerned with space-time derivative estimates of solutions to the fractional Navier-Stokes equations. It is shown that Λ^nαu^(m)_t ∈ L^(2(6α−5))/(4mα+2nα+4 α−5) (0,T; L^2(ℝ^3)) and $ Λ^{n }u^{(m)}_{t} \in L^{\frac{2(6α-5)}{4mα+2n +4 α-5}}~~~~~(0,T; L^{2}(\mathbb{R}^{3}))$. This generalizes a priori bounds for the classical Navier-Stokes system by Duff in [7, Acta Math. 164, 1990] and Boutros and Gibbon's spatial derivative estimates in [1, Nonlinearity 37, 2024]. In addition, we derive that $ u \in L^{\frac{q}{q-3}}~~(0,T;L^{q} (\mathbb{R}^{3}))$ with $ 6\leq q\leq\infty $ and $Λ^{k}u \in L^{\frac{q}{ q(k+1)-3}}~~~(0,T;L^{q} (\mathbb{R}^{3})) $ with $k\geq1, 2\leq q\leq\infty $ in the standard Navier-Stokes equations.
ER  -