In the Haag-Kastler approach to quantum field theory one deals with local nets indexed by bounded open regions of Minkowski spacetime. An important axiom of this approach is that of causality, which says that observables localized in spacelike separated regions of spacetime commute. A causal index set is an abstraction of the index set of bounded open regions that retains the relation induced by the concept of spacelike separation. It can be used to generalize the axiom of causality to nets with different or more general index sets as the one mentioned above. Causal index sets are needed to define the notion of a causal net of algebras.

Definition

A relation $\perp$ on a $\sigma$-bounded poset$I$ is called a causal disjointness relation (and $a, b \in I$ are called causally disjoint if $a \perp b$) if the following properties are satisfied:

(i) $\perp$ is symmetric

(ii) $a \perp b$ and $c \lt b$ implies $a \perp c$

(iii) if $M \subset I$ is bounded from above, then $a \perp b$ for all $a \in M$ implies $sup M \perp b$.

(iv) for every $a \in I$ there is a $b \in I$ with $a \perp b$

A poset with such a relation is called a causal index set.

Examples

One example is explained in the Idea section.

Let $I$ be the poset of finite subspaces of a separableHilbert space. Define $\perp$ by orthogonality of subspaces, then $(I, \perp)$ is a causal index set.

Let $X$ be a countable set and $I$ be its finite power set, that is the collection of finitesubsets of $X$. Set $M \perp N$ iff $M \cap N = \emptyset$, then this defines a causal disjointness relation. This is an example of a causal complement.

Last revised on June 11, 2010 at 09:00:38.
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