Let (M,g)(M,g) be a time-oriented . The chronological future and causal future of p∈Mp\in M are

I+(p)={q∈M:a future-directed timelike curve runs from p to q},I^+(p)=\{q\in M:\text{a future-directed timelike curve runs from \(p\) to \(q\)}\},
J+(p)={p}∪{q∈M:a future-directed [[differential-geometry/causal-curve|causal curve]] runs from p to q}.J^+(p)=\{p\}\cup \{q\in M:\text{a future-directed [[differential-geometry/causal-curve|causal curve]] runs from \(p\) to \(q\)}\}.

The chronological and causal pasts I−(p)I^-(p) and J−(p)J^-(p) are defined with past-directed curves.

For A⊆MA\subseteq M, set

I±(A)=⋃p∈AI±(p),J±(A)=⋃p∈AJ±(p).I^\pm(A)=\bigcup_{p\in A}I^\pm(p), \qquad J^\pm(A)=\bigcup_{p\in A}J^\pm(p).

One always has I±(p)⊆J±(p)I^\pm(p)\subseteq J^\pm(p). The chronological future is open, whereas the causal future need not be closed without additional causal hypotheses.

The intersection J+(p)∩J−(q)J^+(p)\cap J^-(q) is the between pp and qq.

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.