Condensed Matter Physics, 2020, vol. 23, No. 2, 23502
DOI:10.5488/CMP.23.23502
arXiv:1610.01845
Title:
A phase transition in a Curie-Weiss system with binary interactions
Author(s):
 
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Yu.V. Kozitsky
(Institute of Mathematics, Maria Curie-Skłodowska University, Plac Marii Curie-Skłodowskiej 1, Lublin 20-031, Poland),
 
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M.P. Kozlovskii
(Institute for Condensed Matter Physics of the National Academy of Sciences of Ukraine, 1 Svientsitskii St., 79011 Lviv, Ukraine),
 
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O.A. Dobush
(Institute for Condensed Matter Physics of the National Academy of Sciences of Ukraine, 1 Svientsitskii St., 79011 Lviv, Ukraine)
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A single-sort continuum Curie-Weiss system of interacting particles is studied. The particles are placed in the space
d divided into congruent cubic cells.
For a region V ⊂ d
consisting of N ∈ cells, each two particles contained in
V attract each other with intensity J1/N.
The particles contained in the same cell are subject to binary repulsion with intensity J2 > J1. For fixed values of the temperature, the interaction intensities and
the chemical potential, the thermodynamic phase is defined as a probability measure on the space of occupation numbers of cells, determined by a condition, typical to Curie-Weiss
theories. There is proved that the half-plane J1 × chemical potential contains phase coexistence points at which two thermodynamic phases of the system exist.
An equation of state for this system is obtained.
Key words:
equation of state, phase coexistence, mean field
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