Crystal structures and mechanical properties of tungsten monocarbide predicted by first-principles investigations

The crystal structure of tungsten monocarbide (WC) is researched from 0 to 650 GPa through first principles calculations. The results verify that the experimental structure (hP2-WC) with the space group P 6 over bar m2 is the most stable phase in a wide range of pressure. Above 231 GPa, a new stable structure (space group P6(3)/mmc, hP4-WC) is found to be the most stable phase, and it will transform to a CsCl-type phase (cF8-WC) around 582 GPa. Phonon calculations reveal that the hP4-WC phase is dynamically stable and may be a metastable structure at ambient conditions. The cF8-WC phase possesses dynamical stability above 20 GPa. The hP4-WC phase is a low compressible material with a large bulk modulus of 377 GPa at zero pressure. The hardness values of hP2-WC and hP4-WC at zero pressure are 32 and 21 GPa, respectively, while the cF8-WC phase possesses a hardness of 21 GPa at 20 GPa, implying that these phases are potential hard materials. The temperature-pressure phase boundary of WC is obtained by means of the quasi-harmonic approximation method. As the temperature increases, the transition pressure from hP2-WC to hP4-WC remained nearly unchanged. The transition pressure between hP4-WC and cF8-WC decreases with the increasing temperature.

Automated summary

The crystal structure of tungsten monocarbide (WC) is studied at different pressures from 0 to 650 GPa through first principles calculations, revealing the stability of the experimental hP2-WC structure and the discovery of a new stable hP4-WC phase. The hP4-WC phase is found to be dynamically stable and may serve as a potential hard material with a high bulk modulus. The temperature-pressure phase boundary of WC is obtained, showing the transition pressures between different phases as functions of temperature.