Rhenium diboride is occasionally, and controversially, cited as a "
superhard material" due to its high hardness level. However, tested in the asymptotic-hardness region, as recommended for hard and superhard materials, In another study, a fully dense
B4C-ReB2 ceramic composite nanopowder was fabricated by
spark plasma sintering. It has exhibited a
microhardness of 50 ± 3 GPa under a 49 N load in the asymptotic-hardness region and had a 3.2 g/cm3 density, comparable with the hardness and density of the c-BN. The hardness of ReB2 exhibits considerable
anisotropy because of its hexagonal layered
structure, being greatest along the
c axis. Two factors contribute to the high hardness of ReB2: a high density of
valence electrons, and an abundance of short
covalent bonds. Rhenium has one of the highest valence electron densities of any transition metal (476 electrons/nm3, compare to 572 electrons/nm3 for
osmium and 705 electrons/nm3 for diamond). The addition of boron requires only a 5% expansion of the rhenium lattice because the small boron atoms fill the existing spaces between the rhenium atoms. Furthermore, the
electronegativities of rhenium and boron are close enough (1.9 and 2.04 on the
Pauling scale) that they form covalent bonds in which the electrons are shared almost equally. ==See also==