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From Refs. 14 and 15, a tiny reentrant behavior is visible for bulk (formula presented), which, however, has no consequence to the theoretical results shown later
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From Refs. 14 and 15, a tiny reentrant behavior is visible for bulk (formula presented), which, however, has no consequence to the theoretical results shown later.
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The polaronic carriers were also confirmed in extensive non-CO states of doped manganites, see
-
The polaronic carriers were also confirmed in extensive non-CO states of doped manganites, see A.S. Alexandrov, G.M. Zhao, H. Keller, B. Lorenz, Y.S. Wang, and C.W. Chu, Phys. Rev. B 64, 140404(R) (2001) and references therein.
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85038268681
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Apparently, a more complicated model is needed to account for the “in-phase” order along the z axis, which is beyond the scope of this paper
-
Apparently, a more complicated model is needed to account for the “in-phase” order along the z axis, which is beyond the scope of this paper.
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56
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85038340044
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private communication
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85038338871
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The transition temperature is quantitatively overestimated by the MF theory. And it may be again corrected by the incoherent processes, i.e., phonon states are altered when an electron hops [G.D. Mahan, Many Particle Physics (Plenum, New York, 1990), Sec. 6.2], which are ignored in the derivation of Eq. (2) and become notable at high temperatures
-
The transition temperature is quantitatively overestimated by the MF theory. And it may be again corrected by the incoherent processes, i.e., phonon states are altered when an electron hops [G.D. Mahan, Many Particle Physics (Plenum, New York, 1990), Sec. 6.2], which are ignored in the derivation of Eq. (2) and become notable at high temperatures.
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60
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85038281066
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As a similar example, the 2D half-filled Hubbard model has AFM ground state for arbitrarily small on-site interaction
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As a similar example, the 2D half-filled Hubbard model has AFM ground state for arbitrarily small on-site interaction.
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61
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The proof is obvious if three properties of the right-hand side of Eq. (3) are noticed (the (formula presented) factor is removed at (formula presented): (i). It is divergent at (formula presented). (ii). It decreases monotonically with increasing x. (iii). It is always lower than the function (formula presented), which gives (formula presented) at (formula presented)
-
The proof is obvious if three properties of the right-hand side of Eq. (3) are noticed (the (formula presented) factor is removed at (formula presented): (i). It is divergent at (formula presented). (ii). It decreases monotonically with increasing x. (iii). It is always lower than the function (formula presented), which gives (formula presented) at (formula presented).
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62
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85038346900
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For real quantification, it would be better to first elaborate the formulas such as Eq. (3)
-
For real quantification, it would be better to first elaborate the formulas such as Eq. (3).
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63
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85038300045
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For example, the change of t in thin films due to purely geometric factors is discussed, unpublished
-
For example, the change of t in thin films due to purely geometric factors is discussed in Q. Yuan, (unpublished).
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