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

∂𝐒∂t=𝐒∧(∂2𝐒∂x2+∂2𝐒∂y2)+∂u∂x∂𝐒∂y+∂u∂y∂𝐒∂x,

 

 

 

 

(1a)

∂2u∂x2−α2∂2u∂y2=−2α2𝐒⋅(∂𝐒∂x∧∂𝐒∂y).

 

 

 

 

(1b)

Lax representation

The Lax representation

Lt=AL−LA

 

 

 

 

(2)

of the equation is given by

L=Σ∂x+αI∂y,

 

 

 

 

(3a)

A=−2iΣ∂x2+(−iΣx−iαΣyΣ+uyI−α3uxΣ)∂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