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4
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4243563148
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Phys. Rev.P.-G. de Gennes, 118, 141 (1960).
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(1960)
Phys. Rev.
, vol.118
, pp. 141
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9
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0000828413
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Phys. Rev. BA. J. Millis, 53, 8434 (1996).
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(1996)
, vol.53
, pp. 8434
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Millis, A.J.1
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12
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0000785319
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Phys. Rev. BA. J. Millis54, 5405 (1996).
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(1996)
, vol.54
, pp. 5405
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Millis, A.J.1
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22
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85038926085
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Only a particular linear combination of two (Formula presented) states can be reached by hopping which has average energy (Formula presented)
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Only a particular linear combination of two (Formula presented) states can be reached by hopping which has average energy (Formula presented)
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25
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85038888762
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We neglected here smaller anisotropic orbital-dependent terms (Formula presented) that cannot affect the results
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We neglected here smaller anisotropic orbital-dependent terms (Formula presented) that cannot affect the results.
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28
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85038957243
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Note that U and (Formula presented) are defined with respect to the (Formula presented) state, in contrast to other conventions (Refs. 17 and 19
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Note that U and (Formula presented) are defined with respect to the (Formula presented) state, in contrast to other conventions (Refs. 17 and 19).
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29
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85038964184
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Different symmetry-broken states are degenerate at (Formula presented) as in the (Formula presented) model (Ref. 12), revealing a high frustration of magnetic interactions which might lead to a spin liquid with strong orbital correlations. Such quantum behavior is suppressed for the parameters of (Formula presented) with sizable (Formula presented) and because of the large (Formula presented) spins
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Different symmetry-broken states are degenerate at (Formula presented) as in the (Formula presented) model (Ref. 12), revealing a high frustration of magnetic interactions which might lead to a spin liquid with strong orbital correlations. Such quantum behavior is suppressed for the parameters of (Formula presented) with sizable (Formula presented) and because of the large (Formula presented) spins.
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31
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85038932003
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The MF values typically overestimate transition temperatures by a factor close to 1.6; it reduces the used MF value of (Formula presented) to the observed (Formula presented)
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The MF values typically overestimate transition temperatures by a factor close to 1.6; it reduces the used MF value of (Formula presented) to the observed (Formula presented)
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35
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85038895563
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It is plausible that a further extension of the present model by including lattice distortions would allow to explain the easy magnetization axis in (Formula presented)
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It is plausible that a further extension of the present model by including lattice distortions would allow to explain the easy magnetization axis in (Formula presented)
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