Magnetic ordering in inorganic
materials is generally considered to be a mechanism for structures
to stabilize open shells of electrons. The intermetallic phase Mn2Hg5 represents a remarkable exception: its crystal
structure is in accordance with the 18-n bonding
scheme and non-spin-polarized density functional theory (DFT) calculations
show a corresponding pseudogap near its Fermi energy. Nevertheless,
it exhibits strong antiferromagnetic ordering virtually all the way
up to its decomposition temperature. In this Article, we examine how
these two features of Mn2Hg5 coexist through
the development of a DFT implementation of the reversed approximation
Molecular Orbital (raMO) analysis. In the non-spin-polarized electronic
structure, the DFT-raMO approach confirms that Mn2Hg5 adheres to the 18-n rule: its chains of
Mn atoms are linked through isolobal triple bonds, with three electron
pairs being shared at each Mn–Mn contact in one σ-type
and two π-type functions. Because each Mn atom has 6 isolobal
Mn–Mn bonds, it achieves a filled 18-electron count at the
compound’s electron concentration of 18 – 6 = 12 electrons/Mn.
A pseudogap thus occurs at the Fermi energy. Upon the introduction
of antiferromagnetic order, the original pseudogap widens and deepens,
suggesting enhancement of a stabilizing effect already present in
the nonmagnetic state. A raMO analysis reveals that antiferromagnetism
enlarges the gap by allowing diradical character to enter into the
Mn–Mn isolobal π bonds, reminiscent of the dissociation
of a classic covalent bond. Antiferromagnetism is accompanied by residual
bonding in the π system, making Mn2Hg5 a vivid realization of the concept of covalent magnetism.