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PreprintCC BY 4.0arXiv

(In)finiteness of slopes for Monge-Ampère equations at flat boundary pieces

Abstract

On any bounded convex domain Ω⊂ℝn with a d-dimensional flat boundary piece F⊂∂Ω, we consider convex solutions with zero boundary values to the Monge-Ampère equations detD2 u= dist( · ,Aff(F))α, detD2 u=dist( · ,∂Ω)α, detD2 u=(−u)α, where dist stands for Euclidean distance and Aff(F) is the affine hull of F. We show that the threshold of the exponent α∈ℝ for u to have infinite slope at F is α≤ 2d−n. For the first two equations, we also show that no solution exists when α≤ 2d−2n. Moreover, when Ω satisfies the ``exterior cone condition with a d-dimensional ridge'' at F, both thresholds are sharp for the first equation, and the infinite-slope threshold is sharp for the last equation.

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BibTeX
@misc{nie2026infiniteness,
  title = {{(In)finiteness of slopes for Monge-Ampère equations at flat boundary pieces}},
  author = {Xin Nie},
  howpublished = {arXiv},
  year = {2026},
  month = oct,
  doi = {10.48550/arxiv.2610.12165},
  eprint = {2610.12165},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2610.12165},
  note = {CC BY 4.0},
}
RIS
TY  - UNPB
TI  - (In)finiteness of slopes for Monge-Ampère equations at flat boundary pieces
AU  - Xin Nie
PY  - 2026
DA  - 2026/10/09
PB  - arXiv
DO  - 10.48550/arxiv.2610.12165
UR  - https://arxiv.org/abs/2610.12165
AB  - On any bounded convex domain Ω⊂ℝ^n with a d-dimensional flat boundary piece F⊂∂Ω, we consider convex solutions with zero boundary values to the Monge-Ampère equations detD^2 u= dist( · ,Aff(F))^α, detD^2 u=dist( · ,∂Ω)^α, detD^2 u=(−u)^α, where dist stands for Euclidean distance and Aff(F) is the affine hull of F. We show that the threshold of the exponent α∈ℝ for u to have infinite slope at F is α≤ 2d−n. For the first two equations, we also show that no solution exists when α≤ 2d−2n. Moreover, when Ω satisfies the ``exterior cone condition with a d-dimensional ridge'' at F, both thresholds are sharp for the first equation, and the infinite-slope threshold is sharp for the last equation.
ER  -