A self-consistent thermodynamic model is used to calculate the temperature dependences of the heat capacity, the thermal expansion coefficient, the bulk compression modulus, the density, Debye temperature, and the Grüneisen parameter of CoSi in the temperature range 0-1400 K. The calculation results agree well with the existing experimental data and can be used to predict the properties of CoSi in the temperature range that has not been experimentally studied. Cobalt monosilicide is shown to have a significant phonon anharmonicity, which can be caused by an electron-phonon interaction, and this anharmonicity should be taken into account in the simulation of its thermoelectric properties.
INTRODUCTIONCobalt monosilicide CoSi is one of the most promising materials for creating thermogenerators, which is caused by the relatively high efficiency of CoSi-based thermogenerators and the physicochemical and mechanical properties of this compound (which are appropriate for technical applications) [1-3]. Nevertheless, many important thermal and elastic properties of CoSi are poorly understood. For example, the experimental data on the CoSi density are restricted to its room-temperature value, and experimental data on the heat capacity, the elastic moduli, and the thermal expansion coefficient are known for a relatively narrow temperature range [4][5][6][7]. The authors of [7] used the density functional theory (DFT) and the Debye model to calculate the properties of CoSi as functions of temperature and pressure. Nevertheless, the results presented in [7] do not agree with the experimental data quantitatively, which can be caused by the fact that the quasi-harmonic approximation used in [7] cannot take into account the effects related to phonon anharmonicity. However, according to the neutron diffraction data in [8], the phonon spectra of iron or cobalt monosilicide are characterized by an anomalously strong anharmonicity.The purpose of this work is to develop a self-consistent thermodynamic model for CoSi to take into account the influence of phonon anharmonicity on its thermal properties. Using this model, we were able to achieve quantitative agreement with the existing experimental data and to perform a self-consistent simulation of the temperature dependences of the lattice components of the heat capacity, the bulk com-