2021/12/07 by Yannick Sire, Sire, Yannick, Tian Xu +1 · 1 citation
Computer Science · Mathematics · Physics and Astronomy · #Advanced Mathematical Modeling in Engineering #Crystallography and Radiation Phenomena #Differential Geometry (math.DG) #FOS: Mathematics #Spectral Theory in Mathematical Physics
paper · pdf · doi:10.48550/arxiv.2112.03640
openalex publication_date 2021/12/07 · openalex created_date 2025/10/10 · openalex updated_date 2026/07/28
Let M be a closed spin manifold of dimension m≥6 equipped with a Riemannian metric \ig and a spin structure \sa. Let \lm1+(\ig) be the smallest positive eigenvalue of the Dirac operator D\ig on M with respect to a metric \ig conformal to \ig. The Bär-Hijazi-Lott invariant is defined by \lmmin+(M,\ig,\sa)=inf\ig∈[\ig]\lm1+(\ig)\Vol(M,\ig)^(1)/(m). In this paper, we show that \lmmin+(M,\ig,\sa)lt;\lmmin+(Sm,\igSm,\saSm)=\frac m2\Vol(Sm,\igSm)\frac1m provided that \ig is not locally conformally flat. This estimate is a spinorial analogue to an estimate by T. Aubin, solving the Yamabe problem in this setting.