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The quarter-filled case is, as far as Hund's coupling is concerned, of little interest here. However, interesting physics can be found in the presence of a magnetic field (see, for example, Ref. [27])
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We have chosen a fixed ration for J/U, because in typical experiments we expect the bandwidth to be the control parameter (through the variation of pressure); this means it is more natural to change U/W and J/W, but keep J/U fixed
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note
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Neglect of last term in (2) in fact appears to be non-critical. We therefore concentrate of the spin-flip terms in Hund's coupling
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