Abstract

Boron suboxide B6O, the hardest known oxide, has an Rm crystal structure (α-B6O) that can be described as an oxygen-stuffed structure of α-boron, or, equivalently, as a cubic close packing of B12 icosahedra with two oxygen atoms occupying all octahedral voids in it. Here we show a new ground state of this compound at ambient conditions, Cmcm-B6O (β-B6O), which in all quantum-mechanical treatments that we tested comes out to be slightly but consistently more stable. Increasing pressure and temperature further stabilizes it with respect to the known α-B6O structure. β-B6O also has a slightly higher hardness and may be synthesized using different experimental protocols. We suggest that β-B6O is present in mixture with α-B6O, and its presence accounts for previously unexplained bands in the experimental Raman spectrum.

Highlights

  • Boron suboxide B6O, the hardest known oxide, has an R3m crystal structure (α-B6O) that can be described as an oxygen-stuffed structure of α-boron, or, equivalently, as a cubic close packing of B12 icosahedra with two oxygen atoms occupying all octahedral voids in it

  • Superhard materials are used in many applications, from cutting, grinding and drilling tools to wear-resistant coatings[1,2,3]

  • The hardness of α-B6O7 was reported to be in the range 30–45 GPa8,9, making it the hardest known oxide[9,10,11]

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Summary

Results

Our variable-composition evolutionary searches expectedly find B2O3 and B6O to be the only stable compounds in the B-O system. There are several compounds very close to stability - B2O7 (this is a 2D-form of B2O3 intercalated with oxygen molecules) and oxygen-deficient versions of B6O with B6O-like structures and compositions between B and B6O. Cmcm-B6O (β-B6O, see Table 1 for structural parameters), instead of the well-known R3m-B6O (α-B6O)[7,12,13,14], turned out to be the most stable structure at ambient pressure, as shown in Fig. 1; phonon calculations have confirmed its dynamical stability. Structural parameters and some of the physical properties of β-B6O are shown, in comparison with α-B6O and two related forms of pure boron Structural parameters and some of the physical properties of β-B6O are shown in Table 1, in comparison with α-B6O and two related forms of pure boron

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