The concept of a causal complement is suitable to establish a causal disjointness relation on index sets where the indices are subsets of a given set. This generalizes the concept of causal complement of subsets of the Minkowski spacetime, see for example Haag-Kastler vacuum representation.
The concept of causal complement, as the name indicates, a concept related to causality on spacetimes, hence a concept associated with Lorentzian manifolds:
One may abstract away some of the key properties of causal complements on Lorentzian manifolds to obtain a more general concept:
Let be Lorentzian manifold (a spacetime), hence a pseudo-Riemannian manifold with one time-like dimension in each tangent space.
Then for any subset, its causal cone is the subset of all points in which may be joined to a point of by a smooth curve which is everywere timelike or lightlike.
(causal complement of subset of Lorentzian manifold)
For a subset of a Lorentzian manifold, its causal complement is the complement of the causal cone:
The causal complement of the causal complement is called the causal closure. If
then the subset is called a causally closed subset.
Let be an arbitrary set and . An assignment
is called a causal complement if the following conditions hold:
(i)
(ii)
(iii)
A set is causally closed iff .
The set is the causal closure of .
Causal complements are always causally closed. The intersection of two causally closed sets is again a causally closed set. The causal complement of a set may be empty.
A causal disjointness relation on an index set of subsets of a given set can be defined via
if all sets have a causal complement and if
(iv) there is a sequence of mutually different subsets with and .
The latter condition is needed to get a -bounded poset; the -boundedness is part of the definition of a causal index set.
Last revised on April 22, 2023 at 00:31:43. See the history of this page for a list of all contributions to it.