Fluctuational electrodynamics in and out of equilibrium
Iver Brevik, Boris Shapiro, and M\'ario Silveirinha

TL;DR
This paper explores the theory of fluctuation-induced forces, including Casimir-Lifshitz forces and quantum friction, highlighting conceptual issues, novel instability phenomena, and different physical setups involving relative motion and currents.
Contribution
It provides a detailed analysis of quantum friction, addressing conceptual problems, and introduces the possibility of instabilities and radiation emission in weakly dissipative systems.
Findings
Quantum friction may be non-stationary in weakly dissipative systems.
Instability can lead to exponential radiation growth under certain conditions.
Differences in frictional forces arise when bodies are at rest with current flow versus relative motion.
Abstract
Dispersion forces between neutral material bodies are due to fluctuations of the polarization of the bodies. For bodies in equilibrium these forces are often referred to as Casimir-Lifshitz forces. For bodies in relative motion, in addition to the Casimir-Lifshitz force, a lateral frictional force ("quantum friction", in the zero temperature limit) comes into play. The widely accepted theory of the fluctuation induced forces is based on the "fluctuational electrodynamics" , when the Maxwell equations are supplemented by random current sources responsible for the fluctuations of the medium polarization. The first part of our paper touches on some conceptual issues of the theory, such as the dissipation-less limit and the link between Rytov's approach and quantum electrodynamics. We point out the problems with the dissipation-less plasma model (with its unphysical double pole at zero…
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