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3 article(s) from Vanossi, Andrea

Nanotribology

Enrico Gnecco,
Susan Perkin,
Andrea Vanossi and
Ernst Meyer

Beilstein J. Nanotechnol. 2018, 9, 2330–2331, doi:10.3762/bjnano.9.217

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Editorial

Published 28 Aug 2018

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Recent highlights in nanoscale and mesoscale friction

Andrea Vanossi,
Dirk Dietzel,
Andre Schirmeisen,
Ernst Meyer,
Rémy Pawlak,
Thilo Glatzel,
Marcin Kisiel,
Shigeki Kawai and
Nicola Manini

Beilstein J. Nanotechnol. 2018, 9, 1995–2014, doi:10.3762/bjnano.9.190

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Figure 1: a) Scheme of a MoO₃ nanocrystal on MoS₂. The AFM tip is firmly positioned on top on the nanocrystal...

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Figure 2: a) Example of a nanomanipulation during which half of a nanoparticle is scan-imaged, before the tip...

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Figure 3: Dependence of nanoparticle shear stress on the contact area. a) Relative shear stress obtained from...

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Figure 4: Front perspective: a snapshot of a MD-simulated frictional interface between a colloidal monolayer ...

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Figure 5: a) A graphene nanoribbon manipulated along a Au(111) surface. A probing tip lifts the GNR verticall...

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Figure 6: Single-molecule tribology. a) Schematic drawing of the experiment: A single porphyrin molecule is a...

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Figure 7: Non-contact friction experiments of NbSe₂. At certain voltages and distances, one finds dramaticall...

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Figure 8: The “Swiss Nanodragster” (SND), a 4’-(p-tolyl)-2,2’:6’,2”-terpyridine molecule, was moved across an...

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Figure 9: Example of a change of conformation potentially triggered at surfaces. a) Trans (1) and cis (2) iso...

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Review

Published 16 Jul 2018

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Velocity dependence of sliding friction on a crystalline surface

Christian Apostoli,
Giovanni Giusti,
Jacopo Ciccoianni,
Gabriele Riva,
Rosario Capozza,
Rosalie Laure Woulaché,
Andrea Vanossi,
Emanuele Panizon and
Nicola Manini

Beilstein J. Nanotechnol. 2017, 8, 2186–2199, doi:10.3762/bjnano.8.218

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Figure 1: A sketch of the 1D slider-substrate model. The large sphere represents the slider, which moves alon...

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Figure 2: The potential-energy profile experienced by the slider as it moves along a hypothetical chain with ...

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Figure 3: The time dependence (a) and (b) of the slider velocity v_SL and (c) of the chain center of mass v_CM ...

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Figure 4: The dynamical friction force as a function of the damping coefficient γ that fixes the (unphysical)...

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Figure 5: Three snapshots of the instantaneous velocities of a few chain atoms as a function of their positio...

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Figure 6: Dynamic friction force as a function of the slider speed v_SL. For comparison, the horizontal dashed...

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Figure 7: (a): A snapshot of the velocities of the chain particles while the slider, instantly at the vertica...

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Figure 8: The square modulus of the Fourier transforms of the velocities v_j(t), at six subsequent times. Here...

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Figure 9: The time-averaged square modulus of the Fourier transform of the chain velocities, for a few charac...

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Figure 10: The positions (a) and heights (b) of the peaks of [Graphic 31] as functions of v_SL. Panels (c) and (d): detail ...

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Figure 11: A direct comparison of the peak wave vectors of [Graphic 34] , with the dynamic friction F_d as a function of v_SL...

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Figure 12: A scheme of the steps performed to identify the phonons whose phase velocity equals v_SL, and the co...

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Figure 13: The positions of the observed peaks of [Graphic 40] (symbols), compared with the values of k of the phonons who...

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Figure 14: (a): The motion of the slider (solid line) as it is pulled by a spring having elastic constant K_pull...

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Figure 15: For smaller and smaller support velocity v_pull, the maximum elastic force experienced by the slider...

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Full Research Paper

Published 19 Oct 2017

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