2006
DOI: 10.1103/physrevlett.97.136106
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Predictions and Observations of Multiple Slip Modes in Atomic-Scale Friction

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Cited by 139 publications
(139 citation statements)
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“…Before doing so, in order to get a better insight on the problem we will briefly describe some of the main properties of the system for a perfect lattice ͑⑀ =0͒. 4,6,[8][9][10][11][12][13] For this case, the main results are shown in Fig. 2͑a͒ where we present the friction force as a function of the corrugation potential amplitude U o at small velocity ͑v s =10 nm/ s͒.…”
Section: Surface Disorder Without Temperaturementioning
confidence: 99%
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“…Before doing so, in order to get a better insight on the problem we will briefly describe some of the main properties of the system for a perfect lattice ͑⑀ =0͒. 4,6,[8][9][10][11][12][13] For this case, the main results are shown in Fig. 2͑a͒ where we present the friction force as a function of the corrugation potential amplitude U o at small velocity ͑v s =10 nm/ s͒.…”
Section: Surface Disorder Without Temperaturementioning
confidence: 99%
“…In theory, this amplitude can be changed by varying the normal load 10,16 although it is worth noting that a change in the normal load is probably changing other parameters of the system in a nontrivial way. The effect of this disorder is a small change in the potential shape ͑see Fig.…”
Section: Dmentioning
confidence: 99%
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“…Transitions between slip regimes for this system have been systematically investigated by Medyanik et al [2] and can be determined by η = 2π 2 U0 a 2 k ef f ; where η < 1 corresponds to smooth sliding, 1 < η < 4.6 to single slip, 4.6 < η < 7.8 to double slip, and so on. In the Note, the authors introduce a new parameter, η 2 = 2π 2 Uo a 2 k (Eq.…”
mentioning
confidence: 99%