Definition

Let (M,g)(M,g) be a with a . A piecewise C1C^1 curve γ:IM\gamma:I\to M is future-directed causal if, wherever γ˙\dot\gamma exists and is nonzero,

g(γ˙,γ˙)0g(\dot\gamma,\dot\gamma)\leq 0

and γ˙\dot\gamma lies in the chosen future cone. A past-directed causal curve is defined using the past cone. Either is called a causal curve.

A causal curve is timelike if g(γ˙,γ˙)<0g(\dot\gamma,\dot\gamma)<0 wherever its tangent is nonzero, and null if g(γ˙,γ˙)=0g(\dot\gamma,\dot\gamma)=0. Definitions using locally Lipschitz curves impose the same condition almost everywhere and include the piecewise-smooth curves used here.

Future-directed causal and timelike curves define the on spacetime.

References
  1. Barrett O'Neill, Semi-Riemannian Geometry With Applications to Relativity, Academic Press, 1983. Publisher record. Relevant: Chapter 14.
  2. Ettore Minguzzi, “Lorentzian causality theory,” Living Reviews in Relativity 22 (2019), article 3. Journal record.