English

Null Distance and Temporal Functions

Differential Geometry 2025-09-12 v3 General Relativity and Quantum Cosmology

Abstract

The notion of null distance was introduced by Sormani and Vega as part of a broader program to develop a theory of metric convergence adapted to Lorentzian geometry. Given a time function τ\tau on a spacetime (M,g)(M,g), the associated null distance d^τ\hat{d}_\tau is constructed from and closely related to the causal structure of MM. While generally only a semi-metric, d^τ\hat{d}_\tau becomes a metric when τ\tau satisfies the local anti-Lipschitz condition. In this work, we focus on temporal functions, that is, differentiable functions whose gradient is everywhere past-directed timelike. Sormani and Vega showed that the class of C1C^1 temporal functions coincides with that of C1C^1 locally anti-Lipschitz time functions. When a temporal function ff is smooth, its level sets Mt=f1(t)M_t = f^{-1}(t) are spacelike hypersurfaces and thus Riemannian manifolds endowed with the induced metric hth_t. Our main result establishes that, on any level set MtM_t where the gradient f\nabla f has constant norm, the null distance d^f\hat{d}_f is bounded above by a constant multiple of the Riemannian distance dhtd_{h_t}. Applying this result to a smooth regular cosmological time function τg\tau_g -- as introduced by Andersson, Galloway, and Howard -- we prove a theorem confirming a conjecture of Sakovich and Sormani (arXiv:2410.16800, 2025): if the diameters of the level sets Mt=τg1(t)M_t = \tau_g^{-1}(t) shrink to zero as t0t \to 0, then the spacetime exhibits a Big Bang singularity, as defined in their work.

Cite

@article{arxiv.2507.07158,
  title  = {Null Distance and Temporal Functions},
  author = {Andrea Nigri},
  journal= {arXiv preprint arXiv:2507.07158},
  year   = {2025}
}

Comments

28 pages, no figures

R2 v1 2026-07-01T03:53:44.650Z