摘要：Recently, a series of high-purity Ti 3 (Al 1-x Si x )C 2 solid solutions with new compositions (x = 0.0, 0.2, 0.4, 0.6, 0.8 and 1.0) have been reported with interesting mechanical properties. Here, we have employed density functional theory for Ti 3 (Al 1-x Si x )C 2 solid solutions to calculate a wider range of physical properties including structural, electronic, mechanical, thermal and optical. With the increase of x, a decrease of cell parameters is observed. All elastic constants and moduli increase with x. The Fermi level gradually increases, moving towards and past the upper bound of the pseudogap, when the value of x goes from zero to unity, indicating that the structural stability reduces gradually when the amount of Si increases within the Ti 3 (Al 1-x Si x )C 2 system. In view of Cauchy pressure, Pugh's ratio and Poisson's ratio all compositions of Ti 3 (Al 1-x Si x )C 2 are brittle in nature. Comparatively, low Debye temperature, lattice thermal conductivity and minimum thermal conductivity of Ti 3 AlC 2 favor it to be a thermal barrier coating material. High melting temperatures implies that the solid solutions Ti 3 (Al 1-x Si x )C 2 may have potential applications in harsh environments. In the visible region (1.8-3.1 eV), the minimum reflectivity of all compositions for both polarizations is above 45%, which makes them potential coating materials for solar heating reduction.
其他摘要：Abstract Recently, a series of high-purity Ti 3 (Al 1− x Si x )C 2 solid solutions with new compositions ( x = 0.0, 0.2, 0.4, 0.6, 0.8 and 1.0) have been reported with interesting mechanical properties. Here, we have employed density functional theory for Ti 3 (Al 1− x Si x )C 2 solid solutions to calculate a wider range of physical properties including structural, electronic, mechanical, thermal and optical. With the increase of x , a decrease of cell parameters is observed. All elastic constants and moduli increase with x . The Fermi level gradually increases, moving towards and past the upper bound of the pseudogap, when the value of x goes from zero to unity, indicating that the structural stability reduces gradually when the amount of Si increases within the Ti 3 (Al 1− x Si x )C 2 system. In view of Cauchy pressure, Pugh’s ratio and Poisson’s ratio all compositions of Ti 3 (Al 1− x Si x )C 2 are brittle in nature. Comparatively, low Debye temperature, lattice thermal conductivity and minimum thermal conductivity of Ti 3 AlC 2 favor it to be a thermal barrier coating material. High melting temperatures implies that the solid solutions Ti 3 (Al 1− x Si x )C 2 may have potential applications in harsh environments. In the visible region (1.8–3.1 eV), the minimum reflectivity of all compositions for both polarizations is above 45%, which makes them potential coating materials for solar heating reduction.
