NANOSCIENCE – THEORY TO APPLICATION

/ Home
/ SUBMISSION

/ The BJNANO
/ Diamond Open Access
/ Journal Statistics
/ Editorial Board
/ Community
/ Call for papers

/ Latest Articles
/ Most accessed
/ Thematic issues
/ Volumes
/ Authors

/ Alerts

/ TWITTER
/ LINKEDIN
/ Mastodon
/ RSS FEED

Empty search

Article Type

Publication Date Range

Search Tips

This search combines search strings from the content search (i.e. "Full Text", "Author", "Title", "Abstract", or "Keywords") with "Article Type" and "Publication Date Range" using the AND operator.

Search Examples

aromatic	the word “aromatic”
aromatic aldehyde	the word “aromatic” OR “aldehyde”
+aromatic +aldehyde	both words “aromatic” AND “aldehyde”
+aromatic -aldehyde	the word “aromatic” but NOT “aldehyde”
“aromatic aldehyde”	the exact phrase “aromatic aldehyde”
benz*	words which begin with “benz”, such as “benzene” or “benzyl”
benz*yl	words that begin with “benz” and end with “yl”, such as “benzyl” or “benzoyl”
benzyl~	words that are close to the word “benzyl”, such as “benzoyl” (i.e., fuzzy search)

BROWSE
Latest Articles
Most accessed
thematic issues
volumes
authors

BROWSE

Latest Articles Most Accessed Thematic Issues Volumes Authors

Author

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

PDF

Editorial

Published 28 Aug 2018

Full text

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

PDF

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

Jump to Figure 1

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

Jump to Figure 2

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

Jump to Figure 3

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

Jump to Figure 4

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

Jump to Figure 5

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

Jump to Figure 6

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

Jump to Figure 7

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

Jump to Figure 8

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

Jump to Figure 9

Album

Review

Published 16 Jul 2018

Full text

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

PDF

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

Jump to Figure 1

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

Jump to Figure 2

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

Jump to Figure 3

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

Jump to Figure 4

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

Jump to Figure 5

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

Jump to Figure 6

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

Jump to Figure 7

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

Jump to Figure 8

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

Jump to Figure 9

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

Jump to Figure 10

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...

Jump to Figure 11

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

Jump to Figure 12

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

Jump to Figure 13

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

Jump to Figure 14

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

Jump to Figure 15

Album

Full Research Paper

Published 19 Oct 2017

Full text

Other Beilstein-Institut Open Science Activities

/ Help / Support & Contact / Alerts / Privacy Policy / Terms & Conditions / Impressum