Abstract:In this paper we study the dissipative effects and decoherence induced on a particle moving at constant speed in front of a dielectric plate in quantum vacuum, developing a Closed-Time-Path (CTP) integral formulation in order to account for the corrections to these phenomena generated by finite temperatures. We compute the frictional force of the moving particle and find that it contains two different contributions: a pure quantum term due to quantum fluctuations (even present at vanishing temperatures) and a … Show more
“…( 20) always identically vanishes since G (q, R a , 0) = 0 due to the crossing relation [58]. In other words, in the steady state, we always have lim T →0 µ T = 0, which is equivalent to say that at zero temperature the frictional force does not have a linear dependence in velocity [26,28,65]. In empty space, this can be understood as a consequence of the system's Lorentz invariance.…”
Section: Quantum and Thermal Viscositymentioning
confidence: 99%
“…where F the is total electromagnetic drag acting on the atom. Although the viscosity has already been investigated in various contexts [15,[21][22][23][24][25][26][27] -including decoherence [28], thermodynamic considerations [29,30], its connection to Cherenkov [31] and Hawking radiation [32,33] -some interesting and relevant features have been overlooked. In the following, we generalize the earlier findings by incorporating the net transfer of angular momentum from the field to the particle.…”
“…( 20) always identically vanishes since G (q, R a , 0) = 0 due to the crossing relation [58]. In other words, in the steady state, we always have lim T →0 µ T = 0, which is equivalent to say that at zero temperature the frictional force does not have a linear dependence in velocity [26,28,65]. In empty space, this can be understood as a consequence of the system's Lorentz invariance.…”
Section: Quantum and Thermal Viscositymentioning
confidence: 99%
“…where F the is total electromagnetic drag acting on the atom. Although the viscosity has already been investigated in various contexts [15,[21][22][23][24][25][26][27] -including decoherence [28], thermodynamic considerations [29,30], its connection to Cherenkov [31] and Hawking radiation [32,33] -some interesting and relevant features have been overlooked. In the following, we generalize the earlier findings by incorporating the net transfer of angular momentum from the field to the particle.…”
“…Due to the experimental challenges involved in the implementation of precision measurements for the observation of such a small force acting on objects near a surface, there has been lately a set of works devoted to finding favorable conditions for its detection. [ 25–31 ] In refs. [32, 33], authors have investigated the van der Waals friction between graphene and an amorphous SiO 2 substrate.…”
Spatially separated bodies in a relative motion through vacuum experience a tiny friction force known as quantum friction (QF). This force has so far eluded experimental detection due to its small magnitude and short range. Quantitative details revealing traces of the QF in the degradation of the quantum coherence of a particle are presented. Environmentally induced decoherence for a particle sliding over a dielectric sheet can be decomposed into contributions of different signatures: one solely induced by the electromagnetic vacuum in the presence of the dielectric and another induced by motion. As the geometric phase (GP) has been proved to be a fruitful venue of investigation to infer features of the quantum systems, herein it is proposed to use the accumulated GP acquired by a particle as a QF sensor. Furthermore, an innovative experiment designed to track traces of QF by measuring the velocity dependence of corrections to the GP and coherence is proposed. The experimentally viable scheme presented can spark renewed optimism for the detection of non‐contact friction, with the hope that this non‐equilibrium phenomenon can be readily measured soon.
“…Next to an atom or an atom-like system (e.g. a nano-particle) moving near a macroscopic body 50,[61][62][63][64][65][66][67][68][69][70][71][72] , the most common scenarios involve two planar macroscopic bodies 49,[73][74][75][76][77][78] . A related, but slightly different setup consists of rotating particles in vacuum or near other objects [79][80][81][82][83][84] .…”
Section: Introductionmentioning
confidence: 99%
“…This behavior is strictly related to drag effects that Einstein and Hopf have analyzed in their pioneering work 1,86 . Eventually, both thermal and quantum effects have to be considered together when characterizing the full dynamics of an object moving within a complex structured electromagnetic environment at finite temperature 42,71,[87][88][89][90] .…”
When two or more objects move relative to one another in vacuum, they experience a drag force which, at zero temperature, usually goes under the name of quantum friction. This contactless non-conservative interaction is mediated by the fluctuations of the material-modified quantum electrodynamic vacuum and, hence, is purely quantum in nature. Numerous investigations have revealed the richness of the mechanisms at work, thereby stimulating novel theoretical and experimental approaches and identifying challenges as well as opportunities. In this article, we provide an overview of the physics surrounding quantum friction and a perspective on recent developments.
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