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PreprintarXiv licencearXiv

Blow-up analysis and compactness for critical Dirac equations on π•Šn

Abstract

We study blow-up and compactness for the critical nonlinear Dirac equation Dg0ψi = Hi|ψi|2/(nβˆ’1)ψi on π•Šn, nβ‰₯ 3, where g0 is the round metric and Hiβ†’ H>0 in C0(π•Šn). Under a first-threshold bound on the critical mass, we prove that every blowing-up sequence has, after passing to a subsequence, a unique blow-up point p satisfying H(p)=maxπ•ŠnH. The rescaled solutions converge to a ground-state Dirac bubble that carries the entire limiting critical mass. Under local uniform C1 bounds on Hi, we use the Kelvin transform and a second rescaling to prove that p is an isolated simple blow-up point. We also derive sharp pointwise and gradient estimates in cylindrical coordinates and identify the normalized Green limit. If the coefficients converge in C2 near p, the Pohozaev identity yields Hessg0H(p)=0. Consequently, if a positive H∈ C2(π•Šn) satisfies Ξ”g0H(p)<0 at every global maximum, then solutions with critical mass bounded by a level slightly above the first threshold are uniformly bounded in L∞(π•Šn). This bound remains uniform under small C2 perturbations of H.

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BibTeX
@misc{li2026blowup,
  title = {{Blow-up analysis and compactness for critical Dirac equations on $\mathbb S^n$}},
  author = {Ting Li and Zhongwei Tang},
  howpublished = {arXiv},
  year = {2026},
  month = oct,
  doi = {10.48550/arxiv.2610.33507},
  eprint = {2610.33507},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2610.33507},
}
RIS
TY  - UNPB
TI  - Blow-up analysis and compactness for critical Dirac equations on π•Š^n
AU  - Ting Li
AU  - Zhongwei Tang
PY  - 2026
DA  - 2026/10/24
PB  - arXiv
DO  - 10.48550/arxiv.2610.33507
UR  - https://arxiv.org/abs/2610.33507
AB  - We study blow-up and compactness for the critical nonlinear Dirac equation D_g_0ψ_i = H_i|ψ_i|^2/(nβˆ’1)ψ_i on π•Š^n, nβ‰₯ 3, where g_0 is the round metric and H_iβ†’ H>0 in C^0(π•Š^n). Under a first-threshold bound on the critical mass, we prove that every blowing-up sequence has, after passing to a subsequence, a unique blow-up point p satisfying H(p)=max_π•Š^nH. The rescaled solutions converge to a ground-state Dirac bubble that carries the entire limiting critical mass. Under local uniform C^1 bounds on H_i, we use the Kelvin transform and a second rescaling to prove that p is an isolated simple blow-up point. We also derive sharp pointwise and gradient estimates in cylindrical coordinates and identify the normalized Green limit. If the coefficients converge in C^2 near p, the Pohozaev identity yields Hess_g_0H(p)=0. Consequently, if a positive H∈ C^2(π•Š^n) satisfies Ξ”_g_0H(p)<0 at every global maximum, then solutions with critical mass bounded by a level slightly above the first threshold are uniformly bounded in L^∞(π•Š^n). This bound remains uniform under small C^2 perturbations of H.
ER  -