Abstract:This paper presents the first examples of massless relativistic quantum field theories which are interacting and asymptotically complete. These two-dimensional theories are obtained by an application of a deformation procedure, introduced recently by Grosse and Lechner, to chiral conformal quantum field theories. The resulting models may not be strictly local, but they contain observables localized in spacelike wedges. It is shown that the scattering theory for waves in two dimensions, due to Buchholz, is stil… Show more
“…In this subsection we show that any such regular chiral net has a complete particle interpretation in terms of non-interacting Wigner particles. These facts follow from our results in [25], but the argument below is more direct.…”
Section: Vacuum Representations and Asymptotic Completeness A Regulasupporting
confidence: 81%
“…(We demonstrated these facts already in [25] in a different context.) To conclude this subsection, we introduce some other useful concepts which are needed in Theorem 2.11 below: Let us choose some closed subspaces K ± ⊂ H ± , invariant under the action of U , and denote by K + out × K − the linear span of the respective scattering states.…”
Section: Definition 25 (A) If S = I On H Out Then We Say That Thesupporting
confidence: 58%
“…For this purpose we consider a particle weight ψ, whose GNS representation is of type I with atomic center and acts on a separable Hilbert space H π ψ . Making use of formula (2.24) and identifying unitarily each π α,e , acting on W −1 (H α ⊗ Ce), with π α := π α,e 0 acting on K α := W −1 (H α ⊗ Ce 0 ) for some chosen e 0 ∈ B α , we obtain 25) where the r.h.s. acts on α∈I {K α ⊗ K α }.…”
Section: Then We Say That This Family Of Particle Weights Has Supersementioning
confidence: 99%
“…25) for any open, bounded interval I ⊂ R and any t ∈ R. We assume that W gives rise to a non-trivial representation of the group Z 2 , i.e. AdW = id and W 2 = I .…”
Section: Infraparticles With Superselected Direction Of Motionmentioning
Particle aspects of two-dimensional conformal field theories are investigated, using methods from algebraic quantum field theory. The results include asymptotic completeness in terms of (counterparts of) Wigner particles in any vacuum representation and the existence of (counterparts of) infraparticles in any charged irreducible product representation of a given chiral conformal field theory. Moreover, an interesting interplay between the infraparticle's direction of motion and the superselection structure is demonstrated in a large class of examples. This phenomenon resembles the electron's momentum superselection expected in quantum electrodynamics.
“…In this subsection we show that any such regular chiral net has a complete particle interpretation in terms of non-interacting Wigner particles. These facts follow from our results in [25], but the argument below is more direct.…”
Section: Vacuum Representations and Asymptotic Completeness A Regulasupporting
confidence: 81%
“…(We demonstrated these facts already in [25] in a different context.) To conclude this subsection, we introduce some other useful concepts which are needed in Theorem 2.11 below: Let us choose some closed subspaces K ± ⊂ H ± , invariant under the action of U , and denote by K + out × K − the linear span of the respective scattering states.…”
Section: Definition 25 (A) If S = I On H Out Then We Say That Thesupporting
confidence: 58%
“…For this purpose we consider a particle weight ψ, whose GNS representation is of type I with atomic center and acts on a separable Hilbert space H π ψ . Making use of formula (2.24) and identifying unitarily each π α,e , acting on W −1 (H α ⊗ Ce), with π α := π α,e 0 acting on K α := W −1 (H α ⊗ Ce 0 ) for some chosen e 0 ∈ B α , we obtain 25) where the r.h.s. acts on α∈I {K α ⊗ K α }.…”
Section: Then We Say That This Family Of Particle Weights Has Supersementioning
confidence: 99%
“…25) for any open, bounded interval I ⊂ R and any t ∈ R. We assume that W gives rise to a non-trivial representation of the group Z 2 , i.e. AdW = id and W 2 = I .…”
Section: Infraparticles With Superselected Direction Of Motionmentioning
Particle aspects of two-dimensional conformal field theories are investigated, using methods from algebraic quantum field theory. The results include asymptotic completeness in terms of (counterparts of) Wigner particles in any vacuum representation and the existence of (counterparts of) infraparticles in any charged irreducible product representation of a given chiral conformal field theory. Moreover, an interesting interplay between the infraparticle's direction of motion and the superselection structure is demonstrated in a large class of examples. This phenomenon resembles the electron's momentum superselection expected in quantum electrodynamics.
“…In the framework of Wightman field theories, this deformation manifests itself as a deformation of the tensor product of the testfunction algebra [GL08], and later on, the connection to Rieffel's strict deformation quantization [Rie92] was explored [BLS10]. By now, the warped convolution technique has also successfully been applied to the deformation of conformal field theories [DT10] and quantum field theories on curved spacetimes [DLM11].…”
Deformations of quantum field theories which preserve Poincaré covariance and localization in wedges are a novel tool in the analysis and construction of model theories. Here a general scenario for such deformations is discussed, and an infinite class of explicit examples is constructed on the Borchers-Uhlmann algebra underlying Wightman quantum field theory. These deformations exist independently of the space-time dimension, and contain the recently studied warped convolution deformation as a special case. In the special case of two-dimensional Minkowski space, they can be used to deform free field theories to integrable models with non-trivial S-matrix.
Several related operator-algebraic constructions for quantum field theory models on Minkowski spacetime are reviewed. The common theme of these constructions is that of a Borchers triple, capturing the structure of observables localized in a Rindler wedge. After reviewing the abstract setting, we discuss in this framework i) the construction of free field theories from standard pairs, ii) the inverse scattering construction of integrable QFT models on two-dimensional Minkowski space, and iii) the warped convolution deformation of QFT models in arbitrary dimension, inspired from non-commutative Minkowski space.
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