Physics:Ishimori equation

From HandWiki

The Ishimori equation is a partial differential equation proposed by the Japanese mathematician (Ishimori 1984). Its interest is as the first example of a nonlinear spin-one field model in the plane that is integrable (Sattinger Tracy).

Equation

The Ishimori equation has the form

𝐒t=𝐒(2𝐒x2+2𝐒y2)+ux𝐒y+uy𝐒x,

 

 

 

 

(1a)

2ux2α22uy2=2α2𝐒(𝐒x𝐒y).

 

 

 

 

(1b)

Lax representation

The Lax representation

Lt=ALLA

 

 

 

 

(2)

of the equation is given by

L=Σx+αIy,

 

 

 

 

(3a)

A=2iΣx2+(iΣxiαΣyΣ+uyIα3uxΣ)x.

 

 

 

 

(3b)

Here

Σ=j=13Sjσj,

 

 

 

 

(4)

the σi are the Pauli matrices and I is the identity matrix.

Reductions

The Ishimori equation admits an important reduction: in 1+1 dimensions it reduces to the continuous classical Heisenberg ferromagnet equation (CCHFE). The CCHFE is integrable.

Equivalent counterpart

The equivalent counterpart of the Ishimori equation is the Davey-Stewartson equation.

See also

References