English

Lorentzian manifolds with shearfree congruences and K\"ahler-Sasaki geometry

Differential Geometry 2021-01-14 v4 General Relativity and Quantum Cosmology High Energy Physics - Theory

Abstract

We study Lorentzian manifolds (M,g)(M, g) of dimension n4n\geq 4, equipped with a maximally twisting shearfree null vector field pop_o, for which the leaf space S=M/{exptpo}S = M/\{\exp t p_o\} is a smooth manifold. If n=2kn = 2k, the quotient S=M/{exptpo}S = M/\{\exp t p_o\} is naturally equipped with a subconformal structure of contact type and, in the most interesting cases, it is a regular Sasaki manifold projecting onto a quantisable K\"ahler manifold of real dimension 2k22k -2. Going backwards through this line of ideas, for any quantisable K\"ahler manifold with associated Sasaki manifold SS, we give the local description of all Lorentzian metrics gg on the total spaces MM of AA-bundles π:MS\pi: M \to S, A=S1,RA = S^1, \mathbb R, such that the generator of the group action is a maximally twisting shearfree gg-null vector field pop_o. We also prove that on any such Lorentzian manifold (M,g)(M, g) there exists a non-trivial generalized electromagnetic plane wave having pop_o as propagating direction field, a result that can be considered as a generalization of the classical 44-dimensional Robinson Theorem. We finally construct a 2-parametric family of Einstein metrics on a trivial bundle M=R×SM = \mathbb R \times S for any prescribed value of the Einstein constant. If dimM=4\dim M = 4, the Ricci flat metrics obtained in this way are the well-known Taub-NUT metrics.

Keywords

Cite

@article{arxiv.2009.07179,
  title  = {Lorentzian manifolds with shearfree congruences and K\"ahler-Sasaki geometry},
  author = {Dmitri V. Alekseevsky and Masoud Ganji and Gerd Schmalz and Andrea Spiro},
  journal= {arXiv preprint arXiv:2009.07179},
  year   = {2021}
}

Comments

37 pages; in v4, we corrected a sign in (5.1) and, in cascade, made adjustments in the subsequent formulas; the changes correspond to a change of orientation and have no effect in any result; we also improved the presentation in Sections 2 and 4 and added ackowledgments