Stability of the $ω$ structure of transition elements

Properties of the $ω$ structure are investigated for 27 transition elements from the viewpoints of thermodynamical and mechanical stability based on first-principles calculations. The thermodynamical stability of the $ω$ structure is compared with those for the body-centered cubic (BCC), face-centered cubic (FCC), and hexagonal close-packed (HCP) structures. Similarly to the case of those popular crystal structures, the occupation number for $d$ orbitals is found to roughly determine relative energy and volume of the nonmagnetic (NM) $ω$ structure. For the group 4 elements (Ti, Zr, and Hf), the $ω$ structure is almost the lowest in energy among the investigated crystal structures and is also mechanically stable. The $ω$ structure of the group 7 elements (Mn, Tc, and Re) is also mechanically stable. The $ω$ Fe is found to exhibit a complicated magnetic state that is different from the ferromagnetic (FM) and NM ones. This magnetic state is the most favorable among the investigated magnetic states. The $ω$ Fe in this magnetic state is also mechanically stable. Energies of binary alloys composed of the elements in the group 4 and those in the groups 5 and 6 are estimated by linear interpolation, and most of the alloys show concentration ranges where the $ω$ structure is the lowest in energy among the investigated crystal structures.

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