Web Release Date: October 29,
Electron Density Distributions Calculated for the Nickel Sulfides Millerite, Vaesite, and Heazlewoodite and Nickel Metal: A Case for the Importance of Ni-Ni Bond Paths for Electron Transport




and
Departments of Geosciences, Materials Science and Engineering, Chemical Engineering, and Mathematics, Virginia Tech, Blacksburg, Virginia 24061, Department of Geosciences, University of Arizona, Tucson, Arizona 85721, and William R. Wiley Environmental Molecular Sciences Laboratory, Pacific Northwest National Laboratory, Richland, Washington 99352
Received: July 25, 2005
In Final Form: September 20, 2005
Abstract:
Bond paths and the bond critical point properties (the electron density (
) and the Hessian of
at the bond
critical points (bcp's)) have been calculated for the bonded interactions comprising the nickel sulfide minerals
millerite, NiS, vaesite, NiS2, and heazlewoodite, Ni3S2, and Ni metal. The experimental Ni-S bond lengths
decrease linearly as the magnitudes of the properties each increases in value. Bond paths exist between the
Ni atoms in heazlewoodite and millerite for the Ni-Ni separations that match the shortest separation in Ni
metal, an indicator that the Ni atoms are bonded. The bcp properties of the bonded interactions in Ni metal
are virtually the same as those in heazlewoodite and millerite. Ni-Ni bond paths are absent in vaesite where
the Ni-Ni separations are 60% greater than those in Ni metal. The bcp properties for the Ni-Ni bonded
interactions scatter along protractions of the Ni-S bond length-bcp property trends, suggesting that the two
bonded interactions have similar characteristics. Ni-Ni bond paths radiate throughout Ni metal and the metallic
heazlewoodite structures as continuous networks whereas the Ni-Ni paths in millerite, a p,d-metal displaying
ionic and covalent features, are restricted to isolated Ni3 rings. Electron transport in Ni metal and heazlewoodite
is pictured as occurring along the bond paths, which behave as networks of atomic size wires that radiate in
a contiguous circuit throughout the two structures. Unlike heazlewoodite, the electron transport in millerite
is pictured as involving a cooperative hopping of the d-orbital electrons from the Ni3 rings comprising Ni3S9
clusters to Ni3 rings in adjacent clusters via the p-orbitals on the interconnecting S atoms. Vaesite, an insulator
at low temperatures and a doped semiconductor at higher temperatures, lacks Ni-Ni bond paths. The net
charges conferred on the Ni and S atoms are about a quarter of their nominal charges for the atoms in millerite
and vaesite with the net charge on Ni increasing with increasing Ni-S bond length. Reduced net charges are
observed on the Ni atoms in heazlewoodite and are related to its Ni-Ni metal bonded interactions and to the
greater covalent character of its bonds. Local energy density and bond critical point properties of the electron
density distributions indicate that the Ni-S and Ni-Ni bonded interactions are intermediate in character
between ionic and covalent.
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