Schr\"odinger-Feynman quantization and composition of observables in general boundary quantum field theory
Robert Oeckl (UNAM)

TL;DR
This paper introduces a rigorous, functorial quantization scheme for linear and affine field theories within the general boundary formulation, incorporating observables and their composition via path integrals, applicable even without a metric spacetime background.
Contribution
It establishes a new quantization framework combining Schr"odinger and Feynman methods, including a novel way to compose observables through spacetime gluing, extending previous geometric quantization approaches.
Findings
Quantization scheme is equivalent to a holomorphic geometric quantization.
Includes a consistent method for quantizing and composing observables.
Reproduces the correct composition of observables in Minkowski space.
Abstract
We show that the Feynman path integral together with the Schr\"odinger representation gives rise to a rigorous and functorial quantization scheme for linear and affine field theories. Since our target framework is the general boundary formulation, the class of field theories that can be quantized in this way includes theories without a metric spacetime background. We also show that this quantization scheme is equivalent to a holomorphic quantization scheme proposed earlier and based on geometric quantization. We proceed to include observables into the scheme, quantized also through the path integral. We show that the quantized observables satisfy the canonical commutation relations, a feature shared with other quantization schemes also discussed. However, in contrast to other schemes the presented quantization also satisfies a correspondence between the composition of classical…
Peer Reviews
No public reviews on file for this paper yet. If you reviewed it on a platform where reviews are public (OpenReview, ICLR, NeurIPS, ICML), you can paste yours below so the community can read it here.
Videos
No videos yet. Explain this paper in a talk, walkthrough, or lecture? Add one.
