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A few comments on (hyper)k\"ahler geometry

Differential Geometry 2026-03-31 v2 High Energy Physics - Theory Mathematical Physics math.MP

Abstract

In this note, we make two methodical observations. \bullet We prove in a simple explicit way that a necessary and sufficient condition for a K\"ahler manifold to be hyperk\"ahler is hikˉhjlˉΩkˉlˉ = CΩijh_{i\bar k} h_{j\bar l } \Omega^{\bar k \bar l} \ =\ C \Omega_{ij}, where hikˉh_{i\bar k} is a complex metric, Ω\Omega is a symplectic matrix and CC is a positive constant. \bullet The procedure of K\"ahler reduction includes two stages. On the first stage, a K\"ahler manifold of dimension 2n2n is reduced to a (2n1)(2n-1) - dimensional manifold, while on the second stage, one arrives at a K\"ahler manifold of dimension 2(n1)2(n-1). We note that this second stage has the meaning of Hamiltonian reduction. We illustrate the procedure by discussing a simple toy model when R3×S1\mathbb{R}^3 \times S^1 is reduced down to S2S^2. We elucidate also hyperk\"ahler reduction of R7×S1\mathbb{R}^7 \times S^1 down to the Taub-NUT metric.

Keywords

Cite

@article{arxiv.2511.11786,
  title  = {A few comments on (hyper)k\"ahler geometry},
  author = {A. V. Smilga},
  journal= {arXiv preprint arXiv:2511.11786},
  year   = {2026}
}

Comments

Minor corrections. A reference added

R2 v1 2026-07-01T07:38:17.328Z