Mottness denotes the additional ingredient, aside from antiferromagnetic ordering, which is necessary to fully describe a Mott Insulator. In other words, we might write
- antiferromagnetic order + mottness = Mott insulator
Thus, mottness accounts for all of the properties of Mott insulators that cannot be attributed simply to antiferromagnetism.
There are a number of properties of Mott insulators, derived from both experimental and theoretical observations, which cannot be attributed to antiferromagnetic ordering and thus constitute mottness. These properties include
- Spectral weight transfer on the Mott scale
- Vanishing of the single particle Green function along a connected surface in momentum space in the first brillouin zone
- Two sign changes of the Hall coefficient as electron doping goes from to (band insulators have only one sign change at )
- The presence of a charge (with the charge of an electron) boson at low energies
- A pseudogap away from half-filling
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