Journal articles on the topic 'Quantum Vacuum Friction'

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1

Davies, P. C. W. "Quantum vacuum friction." Journal of Optics B: Quantum and Semiclassical Optics 7, no. 3 (March 1, 2005): S40—S46. http://dx.doi.org/10.1088/1464-4266/7/3/006.

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2

Eberlein, Claudia. "Quantum friction across the vacuum." Physics World 11, no. 2 (February 1998): 27–28. http://dx.doi.org/10.1088/2058-7058/11/2/28.

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3

Pendry, J. B. "Shearing the vacuum - quantum friction." Journal of Physics: Condensed Matter 9, no. 47 (November 24, 1997): 10301–20. http://dx.doi.org/10.1088/0953-8984/9/47/001.

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4

Xiong, Xue-Yu, Chun-Yuan Gao, and Ren-Xin Xu. "Spindown of magnetars: quantum vacuum friction?" Research in Astronomy and Astrophysics 16, no. 1 (January 2016): 009. http://dx.doi.org/10.1088/1674-4527/16/1/009.

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5

Xu, Zhujing, Zubin Jacob, and Tongcang Li. "Enhancement of rotational vacuum friction by surface photon tunneling." Nanophotonics 10, no. 1 (September 18, 2020): 537–43. http://dx.doi.org/10.1515/nanoph-2020-0391.

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AbstractWhen a neutral sphere is rotating near a surface in vacuum, it will experience a frictional torque due to quantum and thermal electromagnetic fluctuations. Such vacuum friction has attracted many interests but has been too weak to be observed. Here we investigate the vacuum frictional torque on a barium strontium titanate (BST) nanosphere near a BST surface. BST is a perovskite ferroelectric ceramic that can have large dielectric responses at GHz frequencies. At resonant rotating frequencies, the mechanical energy of motion can be converted to electromagnetic energy through resonant photon tunneling, leading to a large enhancement of the vacuum friction. The calculated vacuum frictional torques at resonances at sub-GHz and GHz frequencies are several orders larger than the minimum torque measured by an optically levitated nanorotor recently, and are thus promising to be observed experimentally. Moreover, we calculate the vacuum friction on a rotating sphere near a layered surface for the first time. By optimizing the thickness of the thin-film coating, the frictional torque can be further enhanced by several times.
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6

Reiche, D., F. Intravaia, and K. Busch. "Wading through the void: Exploring quantum friction and nonequilibrium fluctuations." APL Photonics 7, no. 3 (March 1, 2022): 030902. http://dx.doi.org/10.1063/5.0083067.

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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 and opportunities. In this Perspective, we provide an overview of the physics surrounding quantum friction and a perspective on recent developments.
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7

Coelho, Jaziel G., Jonas P. Pereira, and José C. N. de Araujo. "THE INFLUENCE OF QUANTUM VACUUM FRICTION ON PULSARS." Astrophysical Journal 823, no. 2 (May 26, 2016): 97. http://dx.doi.org/10.3847/0004-637x/823/2/97.

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8

Dupays, A., C. Rizzo, D. Bakalov, and G. F. Bignami. "Quantum Vacuum Friction in highly magnetized neutron stars." EPL (Europhysics Letters) 82, no. 6 (June 2008): 69002. http://dx.doi.org/10.1209/0295-5075/82/69002.

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9

Lombardo, Fernando C., Ricardo S. Decca, Ludmila Viotti, and Paula I. Villar. "Detectable Signature of Quantum Friction on a Sliding Particle in Vacuum." Advanced Quantum Technologies 4, no. 5 (March 31, 2021): 2000155. http://dx.doi.org/10.1002/qute.202000155.

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10

Calogeracos, A., and G. E. Volovik. "Rotational quantum friction in superfluids: Radiation from object rotating in superfluid vacuum." Journal of Experimental and Theoretical Physics Letters 69, no. 4 (February 1999): 281–87. http://dx.doi.org/10.1134/1.568024.

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11

Kuwahara, Takuya, Yun Long, Maria-Isabel De Barros Bouchet, Jean Michel Martin, Gianpietro Moras, and Michael Moseler. "Superlow Friction of a-C:H Coatings in Vacuum: Passivation Regimes and Structural Characterization of the Sliding Interfaces." Coatings 11, no. 9 (September 4, 2021): 1069. http://dx.doi.org/10.3390/coatings11091069.

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A combination of atomistic simulations and vacuum tribometry allows atomic-scale insights into the chemical structure of superlubricious hydrogenated diamond-like carbon (a-C:H) interfaces in vacuum. Quantum molecular dynamics shearing simulations provide a structure-property map of the friction regimes that characterize the dry sliding of a-C:H. Shear stresses and structural properties at the sliding interfaces are crucially determined by the hydrogen content CH in the shear zone of the a-C:H coating. Extremely small CH (below 3 at.%) cause cold welding, mechanical mixing and high friction. At intermediate CH (ranging approximately from 3 to 20 at.%), cold welding in combination with mechanical mixing remains the dominant sliding mode, but some a-C:H samples undergo aromatization, resulting in a superlubricious sliding interface. A further increase in CH (above 20 at.%) prevents cold welding completely and changes the superlubricity mechanism from aromatic to hydrogen passivation. The hydrogen-passivated surfaces are composed of short hydrocarbon chains hinting at a tribo-induced oligomerization reaction. In the absence of cold welding, friction strongly correlates with nanoscale roughness, measured by the overlap of colliding protrusions at the sliding interface. Finally, the atomistic friction map is related to reciprocating friction experiments in ultrahigh vacuum. Accompanying X-ray photoelectron and Auger electron spectroscopy (XPS, XAES) analyses elucidate structural changes during vacuum sliding of a hydrogen-rich a-C:H with 36 at.% hydrogen. Initially, the a-C:H is covered by a nanometer-thick hydrogen-depleted surface layer. After a short running-in phase that results in hydrogen accumulation, superlubricity is established. XPS and XAES indicate a non-aromatic 1–2-nm-thick surface layer with polyethylene-like composition in agreement with our simulations.
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12

Fosco, César D., Fernando C. Lombardo, and Francisco D. Mazzitelli. "Motion-Induced Radiation Due to an Atom in the Presence of a Graphene Plane." Universe 7, no. 5 (May 20, 2021): 158. http://dx.doi.org/10.3390/universe7050158.

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We study the motion-induced radiation due to the non-relativistic motion of an atom, coupled to the vacuum electromagnetic field by an electric dipole term, in the presence of a static graphene plate. After computing the probability of emission for an accelerated atom in empty space, we evaluate the corrections due to the presence of the plate. We show that the effect of the plate is to increase the probability of emission when the atom is near the plate and oscillates along a direction perpendicular to it. On the contrary, for parallel oscillations, there is a suppression. We also evaluate the quantum friction on an atom moving at constant velocity parallel to the plate. We show that there is a threshold for quantum friction: friction occurs only when the velocity of the atom is larger than the Fermi velocity of the electrons in graphene.
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13

Carretero-Palacios, Sol. "Quantum levitation of photonic structures." EPJ Web of Conferences 266 (2022): 07002. http://dx.doi.org/10.1051/epjconf/202226607002.

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The Casimir-Lifshitz force originates from the quantum vacuum fluctuations of the electromagnetic field. This force is especially intense between interacting objects at nanoscale distances, and it can be attractive or repulsive depending on the optical properties of the materials (amongst other parameters). This fundamental phenomenon is at the heart of the malfunctioning of nano- and micro-electromechanical devices (NEMS and MEMS) that integrate many of the gadgets we use in our daily lives. Absolute control over these forces would make it possible to suppress adhesion and friction in these NEMs and MEMs. Here, we will show the possibility of controlling the Casimir-Lifshitz force by tuning the optical properties of the interacting objects. Specifically, we will present diverse examples of quantum levitation based on the Casimir-Lifshitz force of self-standing thin films comprising multilayer structures and films with spatial inhomogeneities (caused by imperfections, pores, inclusions, density variations, etc).
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14

Tsekov, Roumen. "Brownian Emitters." Fluctuation and Noise Letters 15, no. 04 (September 29, 2016): 1650022. http://dx.doi.org/10.1142/s021947751650022x.

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A Brownian harmonic oscillator, which dissipates energy either by friction or via emission of electromagnetic radiation, is considered. This Brownian emitter is driven by the surrounding thermo-quantum fluctuations, which are theoretically described by the fluctuation–dissipation theorem. It is shown how the Abraham–Lorentz force leads to dependence of the half-width on the peak frequency of the oscillator amplitude spectral density. It is found that for the case of a charged particle moving in vacuum at zero temperature, its root-mean-square velocity fluctuation is a universal constant, equal to roughly 1/18 of the speed of light. The relevant Fokker–Planck and Smoluchowski equations are also derived.
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15

Guo, Xin, Kimball A. Milton, Gerard Kennedy, William P. McNulty, Nima Pourtolami, and Yang Li. "Energetics of quantum vacuum friction: Field fluctuations." Physical Review D 104, no. 11 (December 8, 2021). http://dx.doi.org/10.1103/physrevd.104.116006.

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16

Wang, Yang, and Yu Jia. "Quantum dissipation and friction attributed to plasmons." Modern Physics Letters B 36, no. 06 (December 24, 2021). http://dx.doi.org/10.1142/s0217984921505898.

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In this paper, we computed quantum friction of two parallel metal plates separated by a small distance moving with constant relative velocity [Formula: see text]. The plasmons as the internal degrees of freedom living on the two plates are coupled to a vacuum field in the gap between the two plates. We got the in–out quantum action which contained all the dynamical information of the system. Furthermore, we associated the imaginary part of the in–out quantum action with dissipation and frictional force. For the case of dispersionless plasmons, the imaginary part of the in–out quantum action is strongly suppressed as [Formula: see text]. The frictional force exhibits the same feature as [Formula: see text]. The difference is that the frictional force increases as [Formula: see text] and decreases as [Formula: see text]. For the case of dispersive plasmons, there is a threshold for the imaginary part of the in–out quantum action and the frictional force, that is, there is no dissipation when the relative velocity [Formula: see text] is not big enough. We gave a classical argument of the existence of the threshold, and this argument matched the mathematical results.
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17

Guo, Xin, Kimball A. Milton, Gerard Kennedy, William P. McNulty, Nima Pourtolami, and Yang Li. "Energetics of quantum vacuum friction. II. Dipole fluctuations and field fluctuations." Physical Review D 106, no. 1 (July 20, 2022). http://dx.doi.org/10.1103/physrevd.106.016008.

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