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Algebraic quantum field theory

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Axiomatic approach to quantum field theory

Algebraic quantum field theory (AQFT) is an application tolocal quantum physics ofC*-algebra theory. Also referred to as theHaag–Kastleraxiomatic framework forquantum field theory, because it was introduced byRudolf Haag and Daniel Kastler (1964). The axioms are stated in terms of an algebra given for every open set inMinkowski space, and mappings between those.

Haag–Kastler axioms

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LetO{\displaystyle {\mathcal {O}}} be the set of all open and bounded subsets of Minkowski space. An algebraic quantum field theory is defined via a set{A(O)}OO{\displaystyle \{{\mathcal {A}}(O)\}_{O\in {\mathcal {O}}}} ofvon Neumann algebrasA(O){\displaystyle {\mathcal {A}}(O)} on a commonHilbert spaceH{\displaystyle {\mathcal {H}}} satisfying the following axioms:[1]

The net algebrasA(O){\displaystyle {\mathcal {A}}(O)} are calledlocal algebras and the C* algebraA:=OOA(O)¯{\displaystyle {\mathcal {A}}:={\overline {\bigcup _{O\in {\mathcal {O}}}{\mathcal {A}}(O)}}} is called thequasilocal algebra.

Category-theoretic formulation

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LetMink be thecategory ofopen subsets of Minkowski space M withinclusion maps asmorphisms. We are given acovariant functorA{\displaystyle {\mathcal {A}}} fromMink touC*alg, the category ofunital C* algebras, such that every morphism inMink maps to amonomorphism inuC*alg (isotony).

ThePoincaré group actscontinuously onMink. There exists apullback of thisaction, which is continuous in thenorm topology ofA(M){\displaystyle {\mathcal {A}}(M)} (Poincaré covariance).

Minkowski space has acausal structure. If anopen setV lies in thecausal complement of an open setU, then theimage of the maps

A(iU,UV){\displaystyle {\mathcal {A}}(i_{U,U\cup V})}

and

A(iV,UV){\displaystyle {\mathcal {A}}(i_{V,U\cup V})}

commute (spacelike commutativity). IfU¯{\displaystyle {\bar {U}}} is thecausal completion of an open setU, thenA(iU,U¯){\displaystyle {\mathcal {A}}(i_{U,{\bar {U}}})} is anisomorphism (primitive causality).

Astate with respect to a C*-algebra is apositive linear functional over it with unitnorm. If we have a state overA(M){\displaystyle {\mathcal {A}}(M)}, we can take the "partial trace" to get states associated withA(U){\displaystyle {\mathcal {A}}(U)} for each open set via thenetmonomorphism. The states over the open sets form apresheaf structure.

According to theGNS construction, for each state, we can associate aHilbert spacerepresentation ofA(M).{\displaystyle {\mathcal {A}}(M).}Pure states correspond toirreducible representations andmixed states correspond toreducible representations. Each irreducible representation (up toequivalence) is called asuperselection sector. We assume there is a pure state called thevacuum such that the Hilbert space associated with it is aunitary representation of thePoincaré group compatible with the Poincaré covariance of the net such that if we look at thePoincaré algebra, the spectrum with respect toenergy-momentum (corresponding tospacetime translations) lies on and in the positivelight cone. This is the vacuum sector.

QFT in curved spacetime

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More recently, the approach has been further implemented to include an algebraic version ofquantum field theory in curved spacetime. Indeed, the viewpoint of local quantum physics is in particular suitable to generalize therenormalization procedure to the theory of quantum fields developed on curved backgrounds. Several rigorous results concerning QFT in presence of ablack hole have been obtained.[citation needed]

References

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  1. ^Baumgärtel, Hellmut (1995).Operatoralgebraic Methods in Quantum Field Theory. Berlin: Akademie Verlag.ISBN 3-05-501655-6.

Further reading

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External links

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