The stress-energy tensor of an Unruh-DeWitt detector
arXiv:2411.09732 · doi:10.1103/PhysRevD.111.045004
Abstract
We propose a model for a finite-size particle detector, which allows us to derive its stress-energy tensor. This tensor is obtained from a covariant Lagrangian that describes not only the quantum field that models the detector, , but also the systems responsible for its localization: a complex scalar field, , and a perfect fluid. The local interaction between the detector and the complex field ensures the square integrability of the detector modes, while the fluid serves to define the spatial profile of , localizing it in space. We then demonstrate that, under very general conditions, the resulting energy tensor -- incorporating all components of the system -- is physically reasonable and satisfies the energy conditions.
11 pages, 7 figures, revtex 4.2
References in corpus (19)
- Wavepacket detection with the Unruh-DeWitt model
- Spontaneous scalarization
- Quantum Measurement Information as a key to Energy Release from Local Vacuums
- Information transmission without energy exchange
- A detector-based measurement theory for quantum field theory
- Violation of the strong Huygen's principle and timelike signals from the early Universe
- Awaking the vacuum in relativistic stars
- Entanglement amplification between superposed detectors in flat and curved spacetimes
- The vacuum revealed: the final state of vacuum instabilities in compact stars
- Relativistic causality in particle detector models: Faster-than-light signalling and "Impossible measurements"
- Long-range entanglement in the Dirac vacuum
- Experimental Activation of Strong Local Passive States with Quantum Information
- Gravity-induced vacuum dominance
- Fully Relativistic Entanglement Harvesting
- Particle creation due to tachyonic instability in relativistic stars
- Particle Detectors from Localized Quantum Field Theories
- Causality and signalling in non-compact detector-field interactions
- An angular momentum based graviton detector
- Quantum Approach to Bound States in Field Theory