词条 | Landau–Lifshitz model |
释义 |
In solid-state physics, the Landau–Lifshitz equation (LLE), named for Lev Landau and Evgeny Lifshitz, is a partial differential equation describing time evolution of magnetism in solids, depending on 1 time variable and 1, 2, or 3 space variables. Landau–Lifshitz equationThe LLE describes an anisotropic magnet. The equation is described in {{harv|Faddeev|Takhtajan|2007|loc=chapter 8}} as follows: It is an equation for a vector field S, in other words a function on R1+n taking values in R3. The equation depends on a fixed symmetric 3 by 3 matrix J, usually assumed to be diagonal; that is, . It is given by Hamilton's equation of motion for the Hamiltonian (where J(S) is the quadratic form of J applied to the vector S) which is In 1+1 dimensions this equation is In 2+1 dimensions this equation takes the form which is the (2+1)-dimensional LLE. For the (3+1)-dimensional case LLE looks like Integrable reductionsIn general case LLE (2) is nonintegrable. But it admits the two integrable reductions: a) in the 1+1 dimensions, that is Eq. (3), it is integrable b) when . In this case the (1+1)-dimensional LLE (3) turns into the continuous classical Heisenberg ferromagnet equation (see e.g. Heisenberg model (classical)) which is already integrable. See also
References
|title=Landau-Lifshitz Equations |series=Frontiers of Research With the Chinese Academy of Sciences |first=Boling |last=Guo |first2= Shijin |last2=Ding|year=2008 |publisher=World Scientific Publishing Company}}
2 : Magnetic ordering|Partial differential equations |
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