2018
DOI: 10.1088/1367-2630/aaf3d5
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Nanofriction and motion of topological defects in self-organized ion Coulomb crystals

Abstract: We study nanofriction in an ion Coulomb crystal under the presence of a topological defect. We have previously observed signatures of the pinning to sliding transition i.e. the symmetry breaking at the critical point and the existence of a vibrational soft mode. Here we discuss how they depend on the position of the topological defect and how external potentials, such as anharmonic trapping potentials or differential light pressure, can be used to change the defect position. The resulting forces tend to break … Show more

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Cited by 15 publications
(9 citation statements)
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“…Here the soft mode of the pinning to sliding transition exhibited a finite frequency at the critical point, when a finite temperature allowed the system to switch between different minima of the Peierls-Nabarro potential [12,61].…”
Section: Discussionmentioning
confidence: 99%
“…Here the soft mode of the pinning to sliding transition exhibited a finite frequency at the critical point, when a finite temperature allowed the system to switch between different minima of the Peierls-Nabarro potential [12,61].…”
Section: Discussionmentioning
confidence: 99%
“…Systems of optically trapped Brownian particles, where the local temperature can be controlled by modulating the trapping laser, have been experimentally studied in [34,35]. Experimentally, the FK potential (1) has been used to describe coulomb crystals of ions in optical lattices [9][10][11][12]. In particular, in [9] the authors were able to control the nanofriction at the individual-atom level.…”
Section: Discussionmentioning
confidence: 99%
“…On the experimental side, the FK model has been realized by using chains of ions in optical lattices [9][10][11][12], and there has been a recent proposal to realize the model by using Ryndberg atoms [13].…”
Section: Introductionmentioning
confidence: 99%
“…Crucially, due to the presence of the defect, the axial distance in the upper and lower subchains differ. As a result, the kink emulates an incommensurate interface of two particle chains, whose influence on one another is determined by the Coulomb repulsion [34]. For low values of α the defect is captured in the trap center due to its repulsion from the crystal boundaries [36].…”
Section: Aubry Transitionmentioning
confidence: 99%
“…Nanofriction has then been characterized by the forces necessary to dislocate the particles, revealing the absence of a friction force in the sliding regime. A different setup emulates Aubry physics in a self-organized system, that is the two sub-chains of an ion crystal under the presence of a topological defect, which provides the necessary incommensurability between the length scales of the subchains [33,34]. Experiments on this approach have demonstrated the softening of a motional mode at the transition point by measuring its resonance frequency.…”
Section: Introductionmentioning
confidence: 99%