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PreprintCC BY 4.0arXiv

Sign-changing bubbling solutions on polygons for the Brezis-Nirenberg problem in high dimensions

Abstract

We consider the Brezis--Nirenberg problem −Δu = |u|2*−2u + ε u in a smooth bounded domain Ω⊂ ℝN, N ≥ 5, with Dirichlet boundary conditions, where ε > 0 is small. Two multi-peak configurations found in dimension four in \cite{PRV2} persist. In an annulus, for every even k ≥ 2, we construct solutions blowing up at the vertices of a regular k-gon with alternating signs. In the ball, we construct solutions blowing up positively at the vertices of a regular k-gon in a coordinate plane and negatively at those of a regular k-gon in an orthogonal plane, for 2 ≤ k ≤ 5 if N = 5,6 and 2 ≤ k ≤ 4 if N ≥ 7. This range is sharp: for larger k no such solution exists with parameters in a compact set, while otherwise the reduced energy has a unique, non-degenerate critical point.

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BibTeX
@misc{rago2026signchanging,
  title = {{Sign-changing bubbling solutions on polygons for the Brezis-Nirenberg problem in high dimensions}},
  author = {Giuseppe Mario Rago},
  howpublished = {arXiv},
  year = {2026},
  month = oct,
  doi = {10.48550/arxiv.2610.26180},
  eprint = {2610.26180},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2610.26180},
  note = {CC BY 4.0},
}
RIS
TY  - UNPB
TI  - Sign-changing bubbling solutions on polygons for the Brezis-Nirenberg problem in high dimensions
AU  - Giuseppe Mario Rago
PY  - 2026
DA  - 2026/10/19
PB  - arXiv
DO  - 10.48550/arxiv.2610.26180
UR  - https://arxiv.org/abs/2610.26180
AB  - We consider the Brezis--Nirenberg problem −Δu = |u|^2^*−2u + ε u in a smooth bounded domain Ω⊂ ℝ^N, N ≥ 5, with Dirichlet boundary conditions, where ε > 0 is small. Two multi-peak configurations found in dimension four in \cite{PRV2} persist. In an annulus, for every even k ≥ 2, we construct solutions blowing up at the vertices of a regular k-gon with alternating signs. In the ball, we construct solutions blowing up positively at the vertices of a regular k-gon in a coordinate plane and negatively at those of a regular k-gon in an orthogonal plane, for 2 ≤ k ≤ 5 if N = 5,6 and 2 ≤ k ≤ 4 if N ≥ 7. This range is sharp: for larger k no such solution exists with parameters in a compact set, while otherwise the reduced energy has a unique, non-degenerate critical point.
ER  -