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{{For|another Landau–Lifshitz equation describing magnetism|Landau–Lifshitz–Gilbert equation}}
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.


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==Landau–Lifshitz equation==
The 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 '''R'''<sup>1+''n''</sup> taking values in '''R'''<sup>3</sup>. The equation  depends on a fixed symmetric 3 by 3 [[matrix (mathematics)|matrix]] ''J'', usually assumed to be [[Diagonal matrix|diagonal]]; that is, <math>J=\operatorname{diag}(J_{1}, J_{2}, J_{3})</math>. It is given by Hamilton's equation of motion for the [[Hamiltonian mechanics|Hamiltonian]]
 
:<math>H=\frac{1}{2}\int \left[\sum_i\left(\frac{\partial \mathbf{S}}{\partial x_i}\right)^{2}-J(\mathbf{S})\right]\, dx\qquad (1)</math>
 
(where ''J''('''S''') is the quadratic form of ''J'' applied to the vector '''S''')
which is
 
:<math> \frac{\partial \mathbf{S}}{\partial t} = \mathbf{S}\wedge \sum_i\frac{\partial^2 \mathbf{S}}{\partial  x_i^{2}} + \mathbf{S}\wedge J\mathbf{S}.\qquad (2)</math>
 
In 1+1 dimensions this equation is
 
:<math> \frac{\partial \mathbf{S}}{\partial t} = \mathbf{S}\wedge \frac{\partial^2 \mathbf{S}}{\partial  x^{2}} + \mathbf{S}\wedge J\mathbf{S}.\qquad (3)</math>
 
In 2+1 dimensions this equation takes the form
 
:<math> \frac{\partial \mathbf{S}}{\partial t} = \mathbf{S}\wedge \left(\frac{\partial^2 \mathbf{S}}{\partial  x^{2}} + \frac{\partial^2 \mathbf{S}}{\partial  y^{2}}\right)+  \mathbf{S}\wedge J\mathbf{S}\qquad (4)</math>
 
which is the (2+1)-dimensional LLE. For the (3+1)-dimensional case LLE looks like
 
:<math> \frac{\partial \mathbf{S}}{\partial t} = \mathbf{S}\wedge \left(\frac{\partial^2 \mathbf{S}}{\partial  x^{2}} + \frac{\partial^2 \mathbf{S}}{\partial  y^{2}}+\frac{\partial^2 \mathbf{S}}{\partial  z^{2}}\right)+ \mathbf{S}\wedge J\mathbf{S}.\qquad (5)</math>
 
==Integrable reductions==
In 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 <math>J=0</math>. 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==
* [[Nonlinear Schrödinger equation]]
* [[Heisenberg model (classical)]]
* [[Spin wave]]
* [[Micromagnetism]]
* [[Ishimori equation]]
* [[Magnet]]
* [[Ferromagnetism]]
 
==References==
*{{citation|mr=2348643|last= Faddeev|first= Ludwig D.|last2= Takhtajan|first2= Leon A.|title= Hamiltonian methods in the theory of solitons|series= Classics in Mathematics|publisher= Springer|place= Berlin|year= 2007|pages= x+592 | ISBN= 978-3-540-69843-2 }}
*{{citation|ISBN= 978-981-277-875-8
|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}}
* [[Arnold Kosevich|Kosevich A.M.]], Ivanov B.A., Kovalev A.S. Nonlinear magnetization waves. Dynamical and topological solitons. – Kiev: [[Naukova Dumka]], 1988. – 192 p.
 
{{DEFAULTSORT:Landau-Lifshitz model}}
[[Category:Magnetic ordering]]
[[Category:Partial differential equations]]

Latest revision as of 17:25, 31 October 2013

28 year-old Painting Investments Worker Truman from Regina, usually spends time with pastimes for instance interior design, property developers in new launch ec Singapore and writing. Last month just traveled to City of the Renaissance. 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). It is given by Hamilton's equation of motion for the Hamiltonian

H=12[i(Sxi)2J(S)]dx(1)

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

St=Si2Sxi2+SJS.(2)

In 1+1 dimensions this equation is

St=S2Sx2+SJS.(3)

In 2+1 dimensions this equation takes the form

St=S(2Sx2+2Sy2)+SJS(4)

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

St=S(2Sx2+2Sy2+2Sz2)+SJS.(5)

Integrable reductions

In 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 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

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