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.
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{diag}(J1,J2,J3)
H= | 1 |
2 |
\int
\left[\sum | ||||
|
\right)2-J(S)\right]dx (1)
(where J(S) is the quadratic form of J applied to the vector S)which is
\partialS | |
\partialt |
=S\wedge
\sum | ||||||||||||
|
+S\wedgeJS. (2)
In 1+1 dimensions, this equation is
\partialS | |
\partialt |
=S\wedge
\partial2S | |
\partialx2 |
+S\wedgeJS. (3)
In 2+1 dimensions, this equation takes the form
\partialS | |
\partialt |
=S\wedge\left(
\partial2S | |
\partialx2 |
+
\partial2S | |
\partialy2 |
\right)+S\wedgeJS (4)
which is the (2+1)-dimensional LLE. For the (3+1)-dimensional case, the LLE looks like
\partialS | |
\partialt |
=S\wedge\left(
\partial2S | |
\partialx2 |
+
\partial2S | + | |
\partialy2 |
\partial2S | |
\partialz2 |
\right)+S\wedgeJS. (5)
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