Abstract
Hund’s rule is one of the fundamentals of the correlation physics at the atomic level, determining the ground state multiplet of the electrons. In real systems, the electrons hop between the atoms and gain the itinerancy, which is usually described by the band theory. The whole content of theories on correlation is to provide a reliable way to describe the intermediate situation between the two limits. Here we propose an approach toward this goal, i.e., we study the two-atom systems of three \(t_{2g}\) orbitals and see how the Hund’s rule is modified by the transfer integral t between them. It is found that the competition between t and the Hund’s coupling J at each atom determines the crossover from the molecular orbital limit to the strong correlation limit. Especially, our focus is on the generalization of the third rule about the spin-orbit interactions (SOIs), in the presence of the correlation. We have found that there are cases where the effective SOIs are appreciably enhanced by the Hund’s coupling at the filling of four or five electrons. This result provides a useful guideline to realize effectively strong SOI with common and lighter elements, which helps to realize nontrivial electronic states without heavy and rare elements.
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- 1.
This average can be considered as the entanglement of formation \(E(\mathcal {E})\) of an ensemble of pure states \(\mathcal {E} = \{ \psi _\text {AB}^{(k)}, p_k \}\), where \(|{\psi _\text {AB}^{(k)}}\rangle \) is a pure state with probability \(p_k\) (\(k=1, \ldots ,d\), with d being the number of pure states in the ensemble) [30]. The entanglement of formation of the ensemble \(\mathcal {E}\) is defined as the ensemble average of the entanglement entropy of the pure states in \(\mathcal {E}\): \(E(\mathcal {E}) = \sum _{k=1}^d p_k S(\rho _{\text {A},k}) = \sum _{k=1}^d p_k S(\rho _{\text {B},k})\), where \(\rho _{\text {A},k}\) and \(\rho _{\text {B},k}\) are the reduced density matrices for the pure state \(|{\psi _\text {AB}^{(k)}}\rangle \). In our calculation, we consider the average of the entanglement entropy for each degenerate state with equal weight, i.e., the entanglement of formation \(E(\mathcal {E})\) with \(p_1= p_2 = \cdots = p_d\). We note that, when \(d=1\), the entanglement of formation \(E(\mathcal {E})\) is equal to the entanglement entropy S.
References
F. Hund, Z. Phys. 40, 742 (1927)
F. Hund, Z. Phys. 42, 93 (1927)
W. Heitler, F. London, Z. Phys. 44, 455 (1927)
N. Nagaosa, J. Sinova, S. Onoda, A.H. MacDonald, N.P. Ong, Rev. Mod. Phys. 82, 1539 (2010)
S. Murakami, N. Nagaosa, in Comprehensive Semiconductor Science and Technology, ed. by P. Bhattacharya, R. Fornari, H. Kamimura (Elsevier, Amsterdam, 2011), p. 222
M.Z. Hasan, C.L. Kane, Rev. Mod. Phys. 82, 3045 (2010)
X.-L. Qi, S.-C. Zhang, Rev. Mod. Phys. 83, 1057 (2011)
B.J. Kim, H. Jin, S.J. Moon, J.-Y. Kim, B.-G. Park, C.S. Leem, J. Yu, T.W. Noh, C. Kim, S.-J. Oh, J.-H. Park, V. Durairaj, G. Cao, E. Rotenberg, Phys. Rev. Lett. 101, 076402 (2008)
A. Shitade, H. Katsura, J. Kuneš, X.-L. Qi, S.-C. Zhang, N. Nagaosa, Phys. Rev. Lett. 102, 256403 (2009)
G. Jackeli, G. Khaliullin, Phys. Rev. Lett. 102, 017205 (2009)
E. Rashba, Sov. Phys. Solid State 2, 1109 (1960)
K. Yoshida, Theory of Magnetism (Springer, New York, 1996)
S. Raghu, X.-L. Qi, C. Honerkamp, S.-C. Zhang, Phys. Rev. Lett. 100, 156401 (2008)
Y. Zhang, Y. Ran, A. Vishwanath, Phys. Rev. B 79, 245331 (2009)
J. Wen, A. Rüegg, C.-C.J. Wang, G.A. Fiete, Phys. Rev. B 82, 075125 (2010)
M. Kurita, Y. Yamaji, M. Imada, J. Phys. Soc. Jpn. 80, 044708 (2011)
M. Imada, A. Fujimori, Y. Tokura, Rev. Mod. Phys. 70, 1039 (1998)
J.C. Slater, G.F. Koster, Phys. Rev. 94, 1498 (1954)
S. Sugano, Y. Tanabe, H. Kamimura, Multiplets of Transition-Metal Ions in Crystals (Academic Press, New York, 1970)
J. Kanamori, Prog. Theor. Phys. 30, 275 (1963)
C.L. Kane, E.J. Mele, Phys. Rev. Lett. 95, 146802 (2005)
C.L. Kane, E.J. Mele, Phys. Rev. Lett. 95, 226801 (2005)
L. Fu, C.L. Kane, E.J. Mele, Phys. Rev. Lett. 98, 106803 (2007)
H. Isobe, N. Nagaosa, Phys. Rev. B 90, 115122 (2014)
A. Georges, L.D. Medici, J. Mravlje, Annu. Rev. Condens. Matter Phys. 4, 137 (2013)
J.B. Goodenough, J. Phys. Chem. Solids 6, 287 (1958)
J. Kanamori, J. Phys. Chem. Solids 10, 87 (1959)
L. de’ Medici, J. Mravlje, A. Georges, Phys. Rev. Lett. 107, 256401 (2011)
L. Amico, R. Fazio, A. Osterloh, V. Vedral, Rev. Mod. Phys. 80, 517 (2008)
C.H. Bennett, D.P. DiVincenzo, J.A. Smolin, W.K. Wootters, Phys. Rev. A 54, 3824 (1996)
Y. Tokura, Physica C 235–240, 138 (1994)
T. Arima, Y. Tokura, J.B. Torrance, Phys. Rev. B 48, 17006 (1993)
S. Miyasaka, Y. Okimoto, Y. Tokura, J. Phys. Soc. Jpn. 71, 2086 (2002)
T. Nakamura, G. Petzow, L. Gauckler, Mater. Res. Bull. 14, 649 (1979)
A.M. Arévalo-López, E. Castillo-Martínez, M.A. Alario-Franco, J. Phys. Condens. Matter 20, 505207 (2008)
B. Chamberland, Solid State Commun. 5, 663 (1967)
D. Peck, M. Miller, K. Hilpert, Solid State Ion. 123, 59 (1999)
J. Longo, P. Raccah, J. Solid State Chem. 6, 526 (1973)
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Isobe, H. (2017). Generalized Hund’s Rule for Two-Atom Systems. In: Theoretical Study on Correlation Effects in Topological Matter. Springer Theses. Springer, Singapore. https://doi.org/10.1007/978-981-10-3743-6_4
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DOI: https://doi.org/10.1007/978-981-10-3743-6_4
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