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・ Landau's function
・ Landau's problems
・ Landau, Luckman, and Lake
・ Landau-Land
・ Landauer
・ Landauer formula
・ Landauer Point
・ Landauer's principle
・ Landaul
・ Landaulet
・ Landau–Arnstorf railway
・ Landau–Hopf theory of turbulence
・ Landau–Kleffner syndrome
・ Landau–Kolmogorov inequality
・ Landau–Lifshitz equation
Landau–Lifshitz model
・ Landau–Lifshitz–Gilbert equation
・ Landau–Pomeranchuk–Migdal effect
・ Landau–Ramanujan constant
・ Landau–Rohrbach railway
・ Landau–Zener formula
・ Landaville
・ Landavran
・ Landay
・ Landay, Helmand
・ Landazuri
・ Landazuri (disambiguation)
・ Landbay
・ Landbeach
・ Landberk


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Landau–Lifshitz model : ウィキペディア英語版
Landau–Lifshitz model

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 equation==
The LLE describes an anisotropic magnet. The equation is described in 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, J=\operatorname(J_, J_, J_). It is given by Hamilton's equation of motion for the Hamiltonian
:H=\frac\int \left(ウィキペディア(Wikipedia)

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