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8
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0001631591
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T. Chatterji, L P. Regnault, P. Thalmeier, R. Suryanarayanan, G. Dhalenne, and A. Revcolevschi, Phys. Rev. B60, R6965 (1999).
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(1999)
Phys. Rev. B
, vol.60
, pp. R6965
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Chatterji, T.1
Regnault, L.P.2
Thalmeier, P.3
Suryanarayanan, R.4
Dhalenne, G.5
Revcolevschi, A.6
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9
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-
0035914844
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T G. Perring, D T. Adroja, G. Chaboussant, G. Aeppli, T. Kimura, and Y. Tokura, Phys. Rev. Lett.87, 217201 (2001).
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(2001)
Phys. Rev. Lett.
, vol.87
, pp. 217201
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Perring, T.G.1
Adroja, D.T.2
Chaboussant, G.3
Aeppli, G.4
Kimura, T.5
Tokura, Y.6
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10
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-
0036469554
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K. Hirota, S. Ishihara, H. Fujioka, M. Kubota, H. Yoshizawa, Y. Moritomo, Y. Endoh, and S. Maekawa, Phys. Rev. B65, 064414 (2002).
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(2002)
Phys. Rev. B
, vol.65
, pp. 64414
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-
Hirota, K.1
Ishihara, S.2
Fujioka, H.3
Kubota, M.4
Yoshizawa, H.5
Moritomo, Y.6
Endoh, Y.7
Maekawa, S.8
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12
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0035844527
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-
A. Koizumi, S. Miyaki, Y. Kakutani, H. Koizumi, N. Hiraoka, K. Makoshi, N. Sakai, K. Hirota, and Y. Murakami, Phys. Rev. Lett.86, 5589 (2001).
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(2001)
Phys. Rev. Lett.
, vol.86
, pp. 5589
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-
Koizumi, A.1
Miyaki, S.2
Kakutani, Y.3
Koizumi, H.4
Hiraoka, N.5
Makoshi, K.6
Sakai, N.7
Hirota, K.8
Murakami, Y.9
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14
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-
85038331275
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-
We ignore a small difference in the Mn-Mn bond lengths, and thus the intralayer and interlayer hopping on the bonds (formula presented) and (formula presented) are given by the same element
-
We ignore a small difference in the Mn-Mn bond lengths, and thus the intralayer and interlayer hopping on the bonds (formula presented) and (formula presented) are given by the same element t.
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-
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15
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0009523591
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M. Kubota, H. Fujioka, K. Hirota, K. Ohoyama, Y. Moritomo, H. Yoshizawa, and Y. Endoh, J. Phys. Soc. Jpn.69, 1606 (2000);
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(2000)
J. Phys. Soc. Jpn.
, vol.69
, pp. 1606
-
-
Kubota, M.1
Fujioka, H.2
Hirota, K.3
Ohoyama, K.4
Moritomo, Y.5
Yoshizawa, H.6
Endoh, Y.7
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17
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0000081596
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-
The, and (formula presented) parameters are given in, and
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The U and (formula presented) parameters are given in T. Mizokawa and A. Fujimori, Phys. Rev. B54, 5368 (1996).
-
(1996)
Phys. Rev. B
, vol.54
, pp. 5368
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Mizokawa, T.1
Fujimori, A.2
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21
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0001419047
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Like the SU(2) invariant formulation for spins:, and
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Like the SU(2) invariant formulation for spins: R. Frésard and P. Wölfle, Int. J. Mod. Phys. B6, 685 (1992).
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(1992)
Int. J. Mod. Phys. B
, vol.6
, pp. 685
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Frésard, R.1
Wölfle, P.2
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22
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0001010104
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-
The value of (formula presented) is somewhat larger than estimated before; (Refs., and,) for (formula presented) it gives the SE constants (formula presented) and (formula presented) in good agreement with the experimental (formula presented) and (formula presented), and
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The value of (formula presented) is somewhat larger than estimated before; (Refs. 5 and 16) for (formula presented) it gives the SE constants (formula presented) and (formula presented) in good agreement with the experimental (formula presented) and (formula presented) F. Moussa, M. Hennion, G. Biotteau, J. Rodríguez-Carvajal, L. Pinsard, and A. Revcolevschi, Phys. Rev. B60, 12 299 (1999).
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(1999)
Phys. Rev. B
, vol.60
, pp. 12 299
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Moussa, F.1
Hennion, M.2
Biotteau, G.3
Rodríguez-Carvajal, J.4
Pinsard, L.5
Revcolevschi, A.6
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24
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30244465641
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The (formula presented) electron contributions to (formula presented) and (formula presented) depend on the type of occupied (formula presented) orbitals, while the (formula presented) terms depend only on the total electron configuration, as explained in Ref., We have used a Hund’s exchange (formula presented) and (formula presented) for (formula presented) and (formula presented) ions:, and
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The (formula presented) electron contributions to (formula presented) and (formula presented) depend on the type of occupied (formula presented) orbitals, while the (formula presented) terms depend only on the total electron configuration, as explained in Ref. 7. We have used a Hund’s exchange (formula presented) and (formula presented) for (formula presented) and (formula presented) ions: A E. Bocquet, T. Mizokawa, T. Saitoh, H. Namatame, and A. Fujimori, Phys. Rev. B46, 3771 (1992).
-
(1992)
Phys. Rev. B
, vol.46
, pp. 3771
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Bocquet, A.E.1
Mizokawa, T.2
Saitoh, T.3
Namatame, H.4
Fujimori, A.5
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25
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0001400611
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-
The operator (formula presented) in the FM term in Eq. (5) projects on the high-spin state and has the general form (formula presented) for a spin-orbital SE model with spin, and
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The operator (formula presented) in the FM term in Eq. (5) projects on the high-spin state and has the general form (formula presented) for a spin-orbital SE model with spin S: G. Khaliullin and R. Kilian, Phys. Rev. B61, 3494 (2000);
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(2000)
Phys. Rev. B
, vol.61
, pp. 3494
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Khaliullin, G.1
Kilian, R.2
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27
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0034451359
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C D. Ling, J E. Millburn, J F. Mitchell, D N. Argyriou, J. Linton, and H N. Bordallo, Phys. Rev. B62, 15 096 (2000).
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(2000)
Phys. Rev. B
, vol.62
, pp. 15 096
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Ling, C.D.1
Millburn, J.E.2
Mitchell, J.F.3
Argyriou, D.N.4
Linton, J.5
Bordallo, H.N.6
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28
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85038303954
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At small (formula presented) the KR slave-boson approach [Eq. (4)] overestimates the reduction of the (formula presented) kinetic energy due to electron correlation, and gives too low values of (formula presented)
-
At small (formula presented) the KR slave-boson approach [Eq. (4)] overestimates the reduction of the (formula presented) kinetic energy due to electron correlation, and gives too low values of (formula presented)
-
-
-
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29
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-
85038265753
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-
The SE could also include the second-neighbor interlayer interaction (formula presented) along (formula presented) involving the hopping of (formula presented) electrons via (formula presented) orbitals, and improving the agreement with the experiment for (formula presented) (Ref
-
The SE could also include the second-neighbor interlayer interaction (formula presented) along (formula presented) involving the hopping of (formula presented) electrons via (formula presented) orbitals, and improving the agreement with the experiment for (formula presented) (Ref. 9).
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