CHARGE-TRANSFER ENERGY IN COMPUTER MODELING OF STRUCTURE AND PROPERTIES OF MINERALS

Citation
Vs. Urusov et Nn. Eremin, CHARGE-TRANSFER ENERGY IN COMPUTER MODELING OF STRUCTURE AND PROPERTIES OF MINERALS, Physics and chemistry of minerals, 24(5), 1997, pp. 374-383
Citations number
32
Categorie Soggetti
Mineralogy,"Material Science
ISSN journal
03421791
Volume
24
Issue
5
Year of publication
1997
Pages
374 - 383
Database
ISI
SICI code
0342-1791(1997)24:5<374:CEICMO>2.0.ZU;2-1
Abstract
As is known, a variable parameter for partial ionicity is often involv ed in the techniques of modeling structure and properties of inorganic crystals by energy-minimization methods. In such a case, to make a ca lculated energy comparable to experimental estimate (atomization energ y) there is a need to involve an intra-atomic energy term the so-calle d charge-transfer energy (Urusov and Eremin 1995). For this purpose a set of charge-transfer energies for valence states of many elements is compiled. The procedure based on aspiration of equalizing the electro nic levels electronegativities is proposed to estimate the total contr ibution of the charge transfer energy in the cohesive energy of a crys tal. The other prescribed quantities are repulsive potential parameter s which are related to the energetic propertis of valence shells of bo nded atoms. The final potential function consists of an effective Coul omb attraction. repulsion and covalent Morse type term. properly weigh ted. The energy-minimization procedure is performed for various values of the ionicity degree parameter of the crystal under study. Thereaft er the charge-transfer energy correction is introduced in order for th e cohesive energy calculations to be made. The calculations of structu re, energy and elastic properties were performed using the METAPOCS co de with ionicity variation for halides (NaCl, CaF2), oxides (MgO, Al2O 3, SiO2 quartz and SnO2), sulphide ZnS and silicate CaSnSiO5. The resu lting cohesive energies usually agree with experiment much better than those calculated in pure ionic or covalent approximations. As to elas tic properties of crystals under consideration, they are generally fun ctions of the ionicity parameter too and in most instances the predict ed properties at intermediate values of the ionicity degree are in a s atisfactory accordance with experimental data.