Landau–Lifshitz model

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Template:For 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 Template:Harv 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=diag⁡(J1,J2,J3). The LLE is then given by Hamilton's equation of motion for the Hamiltonian

H=12∫[∑i(∂𝐒∂xi)2−J(𝐒)]dx(1)

(where J(S) is the quadratic form of J applied to the vector S) which is

∂𝐒∂t=𝐒∧∑i∂2𝐒∂xi2+𝐒∧J𝐒.(2)

In 1+1 dimensions, this equation is

∂𝐒∂t=𝐒∧∂2𝐒∂x2+𝐒∧J𝐒.(3)

In 2+1 dimensions, this equation takes the form

∂𝐒∂t=𝐒∧(∂2𝐒∂x2+∂2𝐒∂y2)+𝐒∧J𝐒(4)

which is the (2+1)-dimensional LLE. For the (3+1)-dimensional case, the LLE looks like

∂𝐒∂t=𝐒∧(∂2𝐒∂x2+∂2𝐒∂y2+∂2𝐒∂z2)+𝐒∧J𝐒.(5)

Integrable reductions

In the general case LLE (2) is nonintegrable, but it admits two integrable reductions:

a) in 1+1 dimensions, that is Eq. (3), it is integrable
b) when J=0. 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