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

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OP-II-2gas model use, <strong>the</strong>re is no need to support dynamic lists <strong>of</strong> neighbour atoms, but similar listscan be prepared before simulation for each lattice cell and such lists don’t need to berefreshed during simulation. No suggestions about lattice type are made by <strong>the</strong> simulationalgorithm, so <strong>the</strong> model easily can be adopted for any kind <strong>of</strong> crystal.On attempt to execute a diffusion act an atom isselected from <strong>the</strong> list <strong>of</strong> lattice cells with activeatoms (atoms <strong>of</strong> <strong>the</strong> particle which can take part indiffusion process). This list is dynamically updatedon each successful diffusion act and is in actual stateduring <strong>the</strong> whole simulation. The second lattice cellis picked from <strong>the</strong> neighbor list <strong>of</strong> <strong>the</strong> first one andan attempt to change <strong>the</strong>ir content is being doneSupported Pt particle with atoms adsorbedon (111) faceaccording to Boltzmann distribution. This approachgives higher acceptance rate than ma<strong>the</strong>matical diffusion because amount <strong>of</strong> unlikely jumpsfrom <strong>the</strong> middle <strong>of</strong> <strong>the</strong> particle to a free space is reduced. Also in that way <strong>the</strong> system reachesan equilibrium state in a less amount <strong>of</strong> steps in comparison with realistic diffusion.An adsorbed atom forms some spatial configuration with adsorbent atoms. Set <strong>of</strong> suchconfigurations defines adsorption type. It can be adsorption on top, on bridge, on hollow sites,on three or four atoms, on steps or o<strong>the</strong>r defects. For our model this set can be specified ininternal coordinates. For each given configuration a lattice pattern is being built for allpossible orientations in space. Obtained patterns can be effectively matched against <strong>the</strong>lattice. It allows quick search <strong>of</strong> places on <strong>the</strong> simulated particle which are suitable for somekind <strong>of</strong> adsorption. Adsorbed atoms don’t have to be placed in lattice cells, <strong>the</strong>ir position isdetermined by vector beginning form some lattice cell. Length <strong>of</strong> this vector is comparablewith distance between atoms in <strong>the</strong> crystal. Therefore a list <strong>of</strong> adjacent adsorbed atoms can bebuild by enumeration <strong>of</strong> neighbor lattice cells which, as described above, can be done quickly.SimulationsWe have used this model for adsorption simulation on supported Pt nanoparticles withdifferent values <strong>of</strong> pressure and parameters <strong>of</strong> interaction between <strong>the</strong> particle and adsorbate.An influence <strong>of</strong> adsorption on particle form has been investigated.References1. V.I. Elokhin and A.V. Myshlyavtsev, Catalytic Processes over Supported Nanoparticles: Simulations, inDekker Encyclopedia <strong>of</strong> Nanoscience and Nanotechnology, ed. Taylor & Francis, 2004.2. F. Cleri and V. Rosato Phys. Rev. B., 1993, 48, 22-33.78

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