Definition

A time orientation on a is a continuous choice, at every point, of one of the two connected components of the timelike cone. Equivalently, it is represented by a continuous timelike vector field; timelike vectors in the chosen component are future-directed, as are causal vectors in its closure. A manifold admitting such a choice is time-orientable.

For with

q(t,x,y,z)=t2+x2+y2+z2,q(t,x,y,z)=-t^2+x^2+y^2+z^2,

the standard choice declares a timelike vector future-directed when t>0t>0. Its closure contains the future-directed null cone and determines the direction used by .

Transformations

A Lorentz transformation is orthochronous when it preserves the chosen future cone. This property is independent of spatial orientation. Requiring both determinant +1+1 and preservation of time orientation selects the .

Time orientation is additional structure: orientability of the underlying manifold does not imply time-orientability, nor conversely.

References
  1. Barrett O'Neill, Semi-Riemannian Geometry With Applications to Relativity, Academic Press, 1983, §5. Publisher record.
  2. Robert M. Wald, General Relativity, University of Chicago Press, 1984, §8.1. Publisher record.