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Lorentzian bordisms in algebraic quantum field theory
Severin Bunk1, James MacManus2, Alexander Schenkel2
1Department of Physics, Astronomy and Mathematics, University of Hertfordshire, College Lane, Hatfield, AL10 9AB UK.
Every algebraic quantum field theory (AQFT) has an underlying functorial field theory defined on Lorentzian bordisms. This functorial structure captures time evolution but not spatial locality, offering new insights into AQFT.
Area of Science:
- Theoretical physics
- Quantum field theory
- Algebraic quantum field theory
Background:
- Algebraic quantum field theory (AQFT) provides a rigorous framework for quantum field theories.
- Understanding the structure and properties of AQFTs is crucial for theoretical physics.
- The role of spacetime structure, particularly Lorentzian manifolds, in AQFT is an active area of research.
Purpose of the Study:
- To demonstrate that every AQFT possesses an underlying functorial field theory.
- To define this functorial field theory on a globally hyperbolic Lorentzian bordism pseudo-category.
- To explore the implications of this functorial structure for understanding time evolution and spatial locality in AQFT.
Main Methods:
- Development of a functorial field theory framework.
- Utilizing globally hyperbolic Lorentzian bordisms as the category for the functor.
- Comparison of algebraic and functorial descriptions for a free scalar quantum field.
Main Results:
- Every AQFT can be associated with a functorial field theory.
- This functorial theory is naturally defined on a pseudo-category of globally hyperbolic Lorentzian bordisms.
- The functorial field theory encodes the time evolution of the AQFT, distinct from its spatial structure.
Conclusions:
- Globally hyperbolic Lorentzian bordisms are fundamental to the structure of AQFT.
- The functorial perspective offers a new way to understand time evolution in quantum field theory.
- This work provides a detailed comparison of algebraic and functorial descriptions for a concrete example (free scalar field).
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