Lorentzian 2d CFT from the pAQFT perspective

Abstract

We provide a detailed construction of the quantum theory of the massless scalar field on 2-dimensional, globally-hyperbolic (in particular, Lorentzian) manifolds using the framework of perturbative algebraic quantum field theory. From this we subalgebras of observables isomorphic to the Heisenberg and Virasoro algebras on the Einstein cylinder. We also show how the conformal version of general covariance, as first introduced by Pinamonti as an extension of the construction due to Brunetti, Fredenhagen and Verch, may be applied to the concept of natural Lagrangians in order to obtain a simple condition for the conformal covariance of classical dynamics, which is then shown to quantise in the case of a quadratic Lagrangian. We then compare the covariance condition for the stress-energy tensor in the classical and quantum theory in Minkowksi space, obtaining a transformation law dependent on the Schwarzian derivative of the transformed coordinate, in accordance with a well-known result in the Euclidean literature.

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Cited by in corpus (6)

• Snowmass White Paper: The Quest to Define QFT
• Wightman fields for two-dimensional conformal field theories with pointed representation category
• Interacting massless infraparticles in 1+1 dimensions
• Homotopy theory of net representations
• Gravitational null rays: Covariant Quantization and the Dressing Time
• Gluing algebraic quantum field theories on manifolds