Equilibrium properties of two-species reactive lattice gases on random catalytic chains
Autor: | Olivier Bénichou, Dmytro Shapoval, Gleb Oshanin, M. Dudka |
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Přispěvatelé: | Sorbonne Université (SU), Laboratoire de Physique Théorique de la Matière Condensée (LPTMC), Centre National de la Recherche Scientifique (CNRS)-Sorbonne Université (SU) |
Jazyk: | angličtina |
Rok vydání: | 2020 |
Předmět: |
Physics
[PHYS]Physics [physics] Statistical Mechanics (cond-mat.stat-mech) Logarithm FOS: Physical sciences Thermodynamics 01 natural sciences Uncorrelated 3. Good health 010305 fluids & plasmas Catalysis Lattice (order) 0103 physical sciences 010306 general physics Random matrix ComputingMilieux_MISCELLANEOUS Condensed Matter - Statistical Mechanics |
Zdroj: | Physical Review E Physical Review E, American Physical Society (APS), 2020, 102 (3), ⟨10.1103/PhysRevE.102.032121⟩ |
ISSN: | 2470-0045 2470-0053 |
DOI: | 10.1103/PhysRevE.102.032121⟩ |
Popis: | We focus here on the thermodynamic properties of adsorbates formed by two-species $A+B \to \oslash$ reactions on a one-dimensional infinite lattice with heterogeneous "catalytic" properties. In our model hard-core $A$ and $B$ particles undergo continuous exchanges with their reservoirs and react when dissimilar species appear at neighboring lattice sites in presence of a "catalyst." The latter is modeled by supposing either that randomly chosen bonds in the lattice promote reactions (Model I) or that reactions are activated by randomly chosen lattice sites (Model II). In the case of annealed disorder in spatial distribution of a catalyst we calculate the pressure of the adsorbate by solving three-site (Model I) or four-site (Model II) recursions obeyed by the corresponding averaged grand-canonical partition functions. In the case of quenched disorder, we use two complementary approaches to find $\textit{exact}$ expressions for the pressure. The first approach is based on direct combinatorial arguments. In the second approach, we frame the model in terms of random matrices; the pressure is then represented as an averaged logarithm of the trace of a product of random $3 \times 3$ matrices -- either uncorrelated (Model I) or sequentially correlated (Model II). 30 pages, 18 figures |
Databáze: | OpenAIRE |
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