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Bisognano-Wichmann theorem (changes)
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Introduction
## Concepts
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** quantization **
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** quantum mechanical system **, ** quantum probability **
* subsystem
* observables
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* operator algebra , C*-algebra , von Neumann algebra
* local net of observables
* causal locality
* Haag-Kastler axioms
* Wightman axioms
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## Theorems
{#Theorems}
### States and observables
* order-theoretic structure in quantum mechanics
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* Harding-Döring-Hamhalter theorem
* Kochen-Specker theorem
* Bell's theorem
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### Operator algebra
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* cyclic vector , separating vector
* modular theory
* Fell's theorem
* Stone-von Neumann theorem
* Haag's theorem
### Local QFT
* Reeh-Schlieder theorem
* Bisognano-Wichmann theorem
* PCT theorem
* spin-statistics theorem
* DHR superselection theory
* Osterwalder-Schrader theorem ( Wick rotation )
### Perturbative QFT
* Schwinger-Dyson equation
* main theorem of perturbative renormalization
Contents
Idea
In the Haag-Kastler approach to quantum field theory the central object is a local net of operator algebras . The modular theory says that the local algebras have an associated modular group and a modular conjugation (see modular theory ). The result of Bisognano-Wichmann that this page is about, describes the relation of these to the Poincare group .
Abstract
…
Definition
…
The Theorem
Assume a Wightman field theory of a scalar neutral field is such that the smeared field operators generate the local algebras, see Wightman axioms .
Then:
The modular group of the algebra associated with a wedge and the vacuum vector coincides with the unitary representation of the group of Lorentz boosts which maps the wedge onto itself.
The modular conjugation of the wedge W is given by the formula
J W = Θ U ( R W ( π ) )
J_W = \Theta U(R_W(\pi))
Here Θ \Theta denotes the PCT-operator of the Wightman field theory and U ( R W ( π ) ) U(R_W(\pi)) is the unitary representation of the rotation which leaves the characteristic two-plane of the wedge invariant. The angle of rotation is π \pi .
The theory fulfills wedge duality, that is the commutant of the algebra associated to a wedge is the algebra associated to the causal complement of the wedge.
References
The original work is:
Bisognano, J. and Wichmann, E.H.: On the duality condition for a Hermitian scalar field , J. Math. Phys. 16 (1975), 985-1007.
There are a lot of secondary references, one is for example:
Daniele Guido: Modular Theory for the von Neumann Algebras of Local Quantum Physics (arXiv )
Last revised on June 21, 2010 at 13:55:15.
See the history of this page for a list of all contributions to it.