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'''Kugel–Khomskii coupling''' describes a [[coupling]] between the [[rotation|spin]] and [[Atomic orbital|orbital]] [[Degrees of freedom (physics and chemistry)|degrees of freedom]] in a solid; it is named after the Russian physicists [[Kliment I. Kugel]] (Климент Ильич Кугель) and [[Daniel I. Khomskii]] (Daniil I. Khomskii, Даниил И. Хомский). The [[Hamiltonian (quantum mechanics)|Hamiltonian]] used is:
 
<math>H=\frac{t^2}{U}\sum_{\langle i,j\rangle}\left[4\left(\overrightarrow{S_i}\cdot\overrightarrow{S_j}\right)(\tau_i^{\alpha}-\frac{1}{2})(\tau_j^{\alpha}-\frac{1}{2})+(\tau_i^{\alpha}+\frac{1}{2})(\tau_j^{\alpha}+\frac{1}{2})-1\right]</math>
 
==References==
* http://kotliar6.rutgers.edu/udo/prof/profd/papers/prb56_14243.pdf
* [http://dx.doi.org/10.1070/PU1982v025n04ABEH004537 K. I. Kugel and D. I. Khomskii, Sov. Phys. Usp. 25, 231 (1982).]
 
{{DEFAULTSORT:Kugel-Khomskii coupling}}
[[Category:Condensed matter physics]]
 
 
{{condensedmatter-stub}}

Latest revision as of 01:53, 19 March 2013