
TL;DR
This paper clarifies the concept of particles in quantum field theory, especially in curved spacetime and quantum gravity, by distinguishing between global and local particle states and showing their convergence in large detectors.
Contribution
It introduces a definition of local particle states that remains valid in quantum gravity, reconciling different notions of particles in flat and curved spacetime.
Findings
Local particle states are eigenstates of local field operators.
Global and local particle states converge in large detectors in flat space.
The new definition is relevant for quantum gravity applications.
Abstract
Theoretical developments related to the gravitational interaction have questioned the notion of particle in quantum field theory (QFT). For instance, uniquely-defined particle states do not exist in general, in QFT on a curved spacetime. More in general, particle states are difficult to define in a background-independent quantum theory of gravity. These difficulties have lead some to suggest that in general QFT should not be interpreted in terms of particle states, but rather in terms of eigenstates of local operators. Still, it is not obvious how to reconcile this view with the empirically-observed ubiquitous particle-like behavior of quantum fields, apparent for instance in experimental high-energy physics, or "particle"-physics. Here we offer an element of clarification by observing that already in flat space there exist --strictly speaking-- two distinct notions of particles:…
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Taxonomy
TopicsNoncommutative and Quantum Gravity Theories · Quantum Electrodynamics and Casimir Effect · Black Holes and Theoretical Physics
