F. Ercolessi
International School for Advanced Studies
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Featured researches published by F. Ercolessi.
Philosophical Magazine | 1988
F. Ercolessi; Michele Parrinello; Erio Tosatti
Abstract Many well known difficulties associated with the use of two-body forces for the description of metallic systems may be overcome by using an expression for the total energy of the form V = ½Σ ij φ(r ij ) + Σ i U(ni), where n i = Σiρ(r ij ) is a generalized atomic coordination. The three functions φ(r), U(n) and ρ(r) are constructed empirically, by fitting several physical quantities including thermal and surface properties. This simple many-body force scheme can be used in molecular-dynamics simulations with few overheads compared with pair-wise systems. We present our realization for gold and summarize the results of recent structural and dynamical studies of Au surfaces.
Physical Review B | 1995
O. Gulseren; F. Ercolessi; Erio Tosatti
Recent work has raised considerable interest on the nature of thin metallic wires. We have investigated the melting behavior of thin cylindrical Pb wires with the axis along a (110) direction, using molecular dynamics and a well-tested many-body potential. We find that---in analogy with cluster melting---the melting temperature
Surface Science | 1992
H.S. Lim; C. K. Ong; F. Ercolessi
T_m (R)
Surface Science | 1987
M. Garofalo; Erio Tosatti; F. Ercolessi
of a wire with radius
Surface Science | 1999
J.A. Torres; Erio Tosatti; A. Dal Corso; F. Ercolessi; Jorge Kohanoff; F. Di Tolla; Jose M. Soler
R
Surface Science | 1986
F. Ercolessi; Michele Parrinello; Erio Tosatti
is lower than that of a bulk solid,
Surface Science | 1987
F. Ercolessi; A. Bartolini; M. Garofalo; Michele Parrinello; Erio Tosatti
T_m^b
Physical Review Letters | 1997
Franck Celestini; F. Ercolessi; Erio Tosatti
, by
EPL | 1992
G. Bilalbegovic; F. Ercolessi; Erio Tosatti
T_m (R) = T_m^b -c/R
Physical Review Letters | 1995
Di Tolla Fd; F. Ercolessi; Erio Tosatti
. Surface melting effects, with formation of a thin skin of highly diffusive atoms at the wire surface, is observed. The diffusivity is lower where the wire surface has a flat, local (111) orientation, and higher at (110) and (100) rounded areas. The possible relevance to recent results on non-rupturing thin necks between an STM tip and a warm surface is addressed.