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Boreskov Institute of Catalysis of the Siberian Branch of Russian ...

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OP-I-10ADSORPTION OF COMPLEX MOLECULES WITH DIFFERENTORIENTATION IN MONOLAYER ON SQUARE LATTICE.MONTE CARLO AND TRANSFER-MATRIX TECHNIQUESV.F. Fefelov*, V.A. Gorbunov*, A.V. Myshlyavtsev* , **, M.D. Myshlyavtseva**Omsk State Technical University, Omsk, Russia**<strong>Institute</strong> <strong>of</strong> Hydrocarbons Processing SB RAS, Omsk, RussiaThe most <strong>of</strong> <strong>the</strong> studies <strong>of</strong> adsorption are devoted to <strong>the</strong> monomolecular adsorption, but<strong>the</strong> statistics and <strong>the</strong>rmodynamics <strong>of</strong> multisite one is <strong>the</strong> interesting problem to date. Thissituation is mainly associated to three difficulties which make <strong>the</strong> complex moleculesstatistics different from <strong>the</strong> usual single particle statistics [1]. Namely, 1) no statisticalequivalence exists between particles and vacancies, 2) <strong>the</strong> occupation <strong>of</strong> a given lattice siteensures that at least one <strong>of</strong> its nearest-neighbor sites is occupied, and 3) an isolated vacancycannot serve to determining whe<strong>the</strong>r that site can ever become occupied. Moreover, <strong>the</strong>re is aproblem <strong>of</strong> different molecular orientation in adlayer [2]. The aim <strong>of</strong> this study isinvestigation <strong>of</strong> complex molecules adsorption on square lattice with different molecularorientations in adlayer.To describe adsorption <strong>of</strong> complex molecules on homogenous surfaces we used <strong>the</strong>general lattice gas model. One <strong>of</strong> <strong>the</strong> simplest kinds (do not taking into account <strong>the</strong> dimeradsorption) <strong>of</strong> complex molecules which can variously orientate on <strong>the</strong> surface isquadrangular pyramid. Such molecules can adsorb by two different ways: 1) adsorbedmolecule occupies one site (on top adsorption); 2) adsorbed molecule occupies four sites (onfacet adsorption).To take into account own size <strong>of</strong> <strong>the</strong> molecules we involve infinity strong repulsiveinteractions between nearest-neighbor particles (adsorption to nearest-neighbor sites aroundadsorbed molecules is prohibited). The model was studied with grand canonical ensemble.The model parameters are chemical potential μ, temperature T and ∆ – difference between <strong>the</strong>adsorption heat on facet and on top adsorption.One <strong>of</strong> <strong>the</strong> methods used for calculations was transfer-matrix technique. The transfermatrixis generated for stripe cut out from <strong>the</strong> square lattice with M sites along X axis andwith infinity length along Y axis. Along X axis periodic boundary conditions are used. Forour model <strong>the</strong> state <strong>of</strong> <strong>the</strong> surface in whole can be described as set <strong>of</strong> lattice site states, eachones can be in six states. On <strong>the</strong> o<strong>the</strong>r hand, we used <strong>the</strong> standard Monte Carlo method. Thesites were arranged in a square lattice <strong>of</strong> side L (N=L×L), with conventional periodicboundary conditions. With this method phase diagram was made.The multiple-histogram reweighting and finite-size scaling techniques (<strong>the</strong> fourth-orderBinder’s cumulant <strong>of</strong> <strong>the</strong> order parameter) have been used to estimate <strong>the</strong> phase diagram <strong>of</strong>44

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