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Beilstein J. Nanotechnol. 2023, 14, 711–721, doi:10.3762/bjnano.14.57
Figure 1: Left: A particle of mass m is constrained to move along a path (red curve). An axis is assumed so t...
Figure 2: Impact of the passage of a single particle on the angle of a 50-helix. The shaded region denotes th...
Figure 3: Time evolution of the angle of the path ϑ under a current IT = 40, for different mass ratios μ = m/M...
Figure 4: Dependence of the average angular velocity of the helix under a mass current Im = mI for different ...
Figure 5: Time evolution of the angular velocity for a path with ρF = R, where the angular momentum boosts do...
Figure 6: Threshold mass current as a function of the impact velocity for different values of the exit radius...
Figure 7: Velocity dependence of the threshold momentum current . The large-velocity limit is dominated by th...
Figure 8: Velocity dependence of average angular velocity of the path exposed to a mass current Im. For lower...
Figure 9: Threshold mass ratio m/M for an unbound directed motion as a function of the helix length N (δN = 1...
Beilstein J. Nanotechnol. 2016, 7, 533–543, doi:10.3762/bjnano.7.47
Figure 1: Top and side views of water structures on Pb(111) at different coverages, θ. The Pb, O and H atoms ...
Figure 2: Top and side views of minimum-energy water structures on Pb(100) for coverages from 25 to 200%. The...
Figure 3: Top and side views of the energetically most stable water structures on Pb(311) (a), Pb(511) (b) an...
Figure 4: Isosurface plots of charge-density differences upon water adsorption on a) Pb(100) and b) Pb(511). ...
Figure 5: Upper two panels: Snapshots of the AIMD simulation of water layers at a temperature of 140 K on a) ...
Figure 6: Vibrational spectra of the water layer on Pb(111), Pb(100), Pb(311), Pb(511) and Pb(711) derived fr...