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A Quantitative Gidas--Ni--Nirenberg Theorem for the Fractional Laplacian

Abstract

We establish a quantitative Gidas--Ni--Nirenberg theorem for the pure fractional Dirichlet problem (−Δ)s u=k(x)g(u) in B1, u=0 in ℝn∖ B1, 0<s<1. For positive bounded solutions under a two-sided L∞ normalization, we prove 𝒟(u)≤ C 𝒟(k)γ, 0<γ<1, where 𝒟 measures spherical oscillation and outward radial increase. To the best of our knowledge, this provides the first quantitative Gidas--Ni--Nirenberg estimate for the pure fractional Dirichlet problem. The key new ingredient is a shift-uniform, weak Harnack inequality for shifted antisymmetric supersolutions, which overcomes the exterior-tail obstruction in the quantitative moving-plane argument. This mechanism extends to nonseparable nonlinearities.

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BibTeX
@misc{shen2026quantitative,
  title = {{A Quantitative Gidas--Ni--Nirenberg Theorem for the Fractional Laplacian}},
  author = {Qizhen Shen and Jiongduo Xie},
  howpublished = {arXiv},
  year = {2026},
  month = sep,
  doi = {10.48550/arxiv.2609.14618},
  eprint = {2609.14618},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2609.14618},
}
RIS
TY  - UNPB
TI  - A Quantitative Gidas--Ni--Nirenberg Theorem for the Fractional Laplacian
AU  - Qizhen Shen
AU  - Jiongduo Xie
PY  - 2026
DA  - 2026/09/13
PB  - arXiv
DO  - 10.48550/arxiv.2609.14618
UR  - https://arxiv.org/abs/2609.14618
AB  - We establish a quantitative Gidas--Ni--Nirenberg theorem for the pure fractional Dirichlet problem (−Δ)^s u=k(x)g(u) in B_1, u=0 in ℝ^n∖ B_1, 0<s<1. For positive bounded solutions under a two-sided L^∞ normalization, we prove 𝒟(u)≤ C 𝒟(k)^γ, 0<γ<1, where 𝒟 measures spherical oscillation and outward radial increase. To the best of our knowledge, this provides the first quantitative Gidas--Ni--Nirenberg estimate for the pure fractional Dirichlet problem. The key new ingredient is a shift-uniform, weak Harnack inequality for shifted antisymmetric supersolutions, which overcomes the exterior-tail obstruction in the quantitative moving-plane argument. This mechanism extends to nonseparable nonlinearities.
ER  -