algebraic quantum field theory (perturbative, on curved spacetimes, homotopical)
quantum mechanical system, quantum probability
interacting field quantization
A -dynamical system (or -system, for short) is a continuously acted upon by a topological group of -automorphisms.
In quantum mechanics and generally in AQFT, where quantum observables of the theory are self-adjoint operators of (a local net of) -algebras, the global gauge group of the theory is the maximal group of unitary operators that leave all observables invariant, hence algebra of quantum observables equipped with this action of the global gauge group form a -system.
A -system consists of a -algebra , a locally compact group and a continuous homomorphism of into the group of -automorphisms of equipped with the topology of pointwise convergence.
If the algebra is a -algebra only, then some authors call it a -system.
Sometimes the continuity condition is dropped entirely or replaced by some weaker assumption, therefore one should always check what – if any – continuity assumption an author makes.
The fixed point algebra of a -system is . If the fixed point algebra is trivial then acts ergodically.
A state of the algebra is an invariant state if
The set of invariant states is convex, weak- closed and weak- compact (cf. operator topology).
Hellmut Baumgärtel, Manfred Wollenberg; chapter 6 of: Causal nets of operator algebras — Mathematical aspects of algebraic quantum field theory, Mathematische Lehrbücher und Monographien. II. Abteilung: Mathematische Monographien 80, Akademie Verlag (1992) [zbmath:0749.46038]
Gert K. Pedersen; chapter 6 in: Pullback and pushout constructions in -algebra theory, J. Funct. Analysis 167 (1999) 243–344 [doi:10.1006/jfan.1999.3456, pdf]
Last revised on April 9, 2026 at 13:08:24. See the history of this page for a list of all contributions to it.