nLab
future

Past and future

Idea

The past of any physical event (object, system, etc) consists of everything that might (by the principles of causality?) have potentially influenced that event; while its future consists of everything that it might potentially influence.

Definitions

Let (X,g,o) be a spacetime, that is a Lorentzian manifold (X,g) equipped with time-orientation?. This time-orientation consists precisely of specification of which timelike and lightlike curves are future-directed (and which are complementarily past-directed).

Let x be a point in this spacetime. Then:

  • the future of x is the subset J +(x) of all points of X connected to x by a future-directed timelike or lightlike curve starting at x;

  • the past of x is the subset J (x) of all points of X connected to x by a future-directed timelike or lightlike curve ending at x.

Let A be a more general subset of this spacetimes. Then:

  • the future of A is the subset J +(A) defined as the union of J +(x) for all xA;

  • the past of A is the subset J (A) defined as the union of J (x) for all xA.

Properties

A Cauchy surface Σ in (X,g) is a minimal subset of X with the property that X is the union of the future and past of Σ. (Does this suffice to define Cauchy surfaces in the case of a Lorentzian manifold that admits a time-orientation?)

The operations J + and J are (separately) Moore closures on the power set of X. Stated explicitly (for J +):

  • the future of A contains A;
  • the future of the future of A is simply the future of A;
  • if A contains B, then the future of A contains the future of B.

Variations

Sometimes one wants to remove x itself from J +(x) and J (x) (or more precisely, to include x only in the case of a closed timelike curve through x). However, the operations J + and J are not quite as mathematically well-behaved in this case. (Note that J +(A) may still intersect A, or even contain all of A, even in the absence of closed timelike curves.)

Revised on July 9, 2011 23:01:05 by Toby Bartels (76.85.192.183)