Quantization of the Electromagnetic Field in Non-dispersive Polarizable Moving Media above the Cherenkov Threshold
arXiv:1307.0130 · doi:10.1103/PhysRevA.88.043846
Abstract
We quantize the macroscopic electromagnetic field in a system of non-dispersive polarizable bodies moving at constant velocities possibly exceeding the Cherenkov threshold. It is shown that in general the quantized system is unstable and neither has a ground state nor supports stationary states. The quantized Hamiltonian is written in terms of quantum harmonic oscillators associated with both positive and negative frequencies, such that the oscillators associated with symmetric frequencies are coupled by an interaction term that does not preserve the quantum occupation numbers. Moreover, in the linear regime the amplitudes of the fields may grow without limit provided the velocity of the moving bodies is enforced to be constant. This requires the application of an external mechanical force that effectively pumps the system.
52 pages, under review
References in corpus (4)
Cited by in corpus (12)
- Negative Landau damping in bilayer graphene
- Theory of Quantum Friction
- Cherenkov friction on a neutral particle moving parallel to a dielectric
- Revisiting the Abraham-Minkowski Dilemma
- Wave Instabilities and Unidirectional Light Flow in a Cavity with Rotating Walls
- Spontaneous Parity-Time Symmetry Breaking in Moving Media
- Casimir friction at zero and finite temperatures
- Nonequilibrium quantum fluctuations of a dispersive medium: Spontaneous emission, photon statistics, entropy generation, and stochastic motion
- Negative spontaneous emission by a moving two-level atom
- Stable-to-unstable transition in quantum friction
- Quantum Friction near the Instability Threshold
- Parametric instability in a magnomechanical system