**algebraic quantum field theory** (perturbative, on curved spacetimes, homotopical)

**quantum mechanical system**, **quantum probability**

**interacting field quantization**

Duality for nets of von Neumann algebras is a concept that was introduced for local nets in the Haag-Kastler approach to quantum field theory. Many results of this approach need some sort of duality in the sense described here or close to it as a precondition.

Let $(M_k)$ be a net of von Neumann algebras with a causal index set $I$ that is a causal net of algebras. Let $R$ be the global algebra of the net, that is

$R = (\bigcup_k M_k){''}$

An index $i \in I$ satisfies **duality** if

$M_i = (\bigcup_{j \perp i} M_j)' \bigcap R = (\bigcap_{j \perp i} M_j^') \bigcap R = \bigcap_{j \perp i} M^c_j$

Here $M^c_j$ is the relative commutant of $M_j$ with respect to $R$.

The net is called **dual** if every index is dual i.e. satisfies duality.

A weaker concept is that of **essentially dual**:

Define an extension $(\hat M_k)$ of the net $(M_k)$ via

$\hat M_i = (\bigcup_{j \perp i} M_j)'$

This extension is not necessarily a causal net anymore. If it is, then it is dual by definition. The net $(M_k)$ is **essentially dual**, if the extended net $(\hat M_k)$ is dual, which is true iff $(\hat M_k)$ is causal.

The net $(M_k)$ is called **maximal** if there is no proper extension which satisfies the causality condition?.

A Haag-Kastler vacuum representation satisfies **Haag duality** if every double cone aka diamond is a dual index. The reason for this relaxation is that full duality of every index is often too restrictive, so that the less restrictive Haag duality plays an important role in the theory.

Let $J_0$ be the index set of diamonds, a Haag-Kastler vacuum representation is **essentially Haag dual** if the net $M(J_0)$ (that is the original net restricted to diamonds as indices) is essentially dual.

Last revised on July 9, 2011 at 13:42:19. See the history of this page for a list of all contributions to it.