scholarly journals Intrinsic long-range bond-order potential for carbon: Performance in Monte Carlo simulations of graphitization

2003 ◽  
Vol 68 (2) ◽  
Author(s):  
J. H. Los ◽  
A. Fasolino
Keyword(s):  
Monte Carlo ◽  
Monte Carlo Simulations ◽  
Long Range ◽  
Bond Order ◽  
Bond Order Potential ◽  
Carbon Performance

scholarly journals Improved long-range reactive bond-order potential for carbon. I. Construction

2005 ◽  
Vol 72 (21) ◽  
Author(s):  
Jan H. Los ◽  
Luca M. Ghiringhelli ◽  
Evert Jan Meijer ◽  
A. Fasolino
Keyword(s):  
Long Range ◽  
Bond Order ◽  
Bond Order Potential

scholarly journals Improved long-range reactive bond-order potential for carbon. II. Molecular simulation of liquid carbon

2005 ◽  
Vol 72 (21) ◽  
Author(s):  
Luca M. Ghiringhelli ◽  
Jan H. Los ◽  
A. Fasolino ◽  
Evert Jan Meijer
Keyword(s):  
Molecular Simulation ◽  
Long Range ◽  
Bond Order ◽  
Liquid Carbon ◽  
Bond Order Potential

Controlling the Long-Range Corrections in Atomistic Monte Carlo Simulations of Two-Phase Systems

2015 ◽  
Vol 11 (10) ◽  
pp. 4573-4585 ◽  
Author(s):  
Florent Goujon ◽  
Aziz Ghoufi ◽  
Patrice Malfreyt ◽  
Dominic J. Tildesley
Keyword(s):  
Monte Carlo ◽  
Monte Carlo Simulations ◽  
Long Range ◽  
Two Phase ◽  
Phase Systems

scholarly journals LONG RANGE CHROMOMAGNETIC FIELDS AT HIGH TEMPERATURE

2011 ◽  
Vol 26 (27n28) ◽  
pp. 4831-4843 ◽  
Author(s):  
S. ANTROPOV ◽  
M. BORDAG ◽  
V. DEMCHIK ◽  
V. SKALOZUB
Keyword(s):  
Monte Carlo ◽  
High Temperature ◽  
Magnetic Flux ◽  
Monte Carlo Simulations ◽  
Long Range ◽  
Dyson Equation ◽  
Polarization Tensor ◽  
Chromomagnetic Field ◽  
Magnetic Mass ◽  
The One

The magnetic mass of neutral gluons in Abelian chromomagnetic field at high temperature is calculated in SU(2) gluodynamics. It is noted that such fields are spontaneously generated at high temperature. The mass is computed either from the Schwinger–Dyson equation accounting for the one-loop polarization tensor or in Monte Carlo simulations on a lattice. In latter case, an average magnetic flux penetrating a plaquette is measured for a number of lattices. Both calculations are in agreement with each other and result in zero magnetic mass. Some applications of the results obtained are discussed.

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