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Fixed-spinor radial solutions of a perturbed Euclidean spinorial Yamabe equation

Abstract

We study the perturbed Euclidean spinorial Yamabe equation Dgℝnψ = n/2(1+ε K(x)) |ψ|2*−2ψ on ℝn, n≥2,where 2*:=2n/(n−1), ε>0 is a small parameter and K is a prescribed radial function. We establish a finite-dimensional reduction within a radial spinor space determined by a fixed unit spinor, reducing the problem to the analysis of a function of the dilation parameter. Under suitable assumptions on K, we obtain explicit existence criteria for solutions with this prescribed spinorial structure, together with a multiplicity criterion yielding solutions associated with distinct scales. These criteria are expressed in terms of the behavior of K at the origin and weighted integral quantities.

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BibTeX
@misc{li2026fixedspinor,
  title = {{Fixed-spinor radial solutions of a perturbed Euclidean spinorial Yamabe equation}},
  author = {Ting Li and Zhongwei Tang and Yuhang Zhang},
  howpublished = {arXiv},
  year = {2026},
  month = oct,
  doi = {10.48550/arxiv.2610.21471},
  eprint = {2610.21471},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2610.21471},
}
RIS
TY  - UNPB
TI  - Fixed-spinor radial solutions of a perturbed Euclidean spinorial Yamabe equation
AU  - Ting Li
AU  - Zhongwei Tang
AU  - Yuhang Zhang
PY  - 2026
DA  - 2026/10/15
PB  - arXiv
DO  - 10.48550/arxiv.2610.21471
UR  - https://arxiv.org/abs/2610.21471
AB  - We study the perturbed Euclidean spinorial Yamabe equation D_g_ℝ^nψ = n/2(1+ε K(x)) |ψ|^2^*−2ψ on ℝ^n, n≥2,where 2^*:=2n/(n−1), ε>0 is a small parameter and K is a prescribed radial function. We establish a finite-dimensional reduction within a radial spinor space determined by a fixed unit spinor, reducing the problem to the analysis of a function of the dilation parameter. Under suitable assumptions on K, we obtain explicit existence criteria for solutions with this prescribed spinorial structure, together with a multiplicity criterion yielding solutions associated with distinct scales. These criteria are expressed in terms of the behavior of K at the origin and weighted integral quantities.
ER  -