Ishimori equation

The Ishimori equation (IE) 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 & Venakides (1991, p. 78).

Equation

The Ishimori Equation has the form

 \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)+  \frac{\partial u}{\partial x}\frac{\partial \mathbf{S}}{\partial  y} +  \frac{\partial u}{\partial y}\frac{\partial \mathbf{S}}{\partial  x},\qquad (1a)
 \frac{\partial^2 u}{\partial x^2}-\alpha^2 \frac{\partial^2 u}{\partial y^2}=-2\alpha^2  \mathbf{S}\cdot\left(\frac{\partial \mathbf{S}}{\partial  x}\wedge \frac{\partial \mathbf{S}}{\partial  y}\right).\qquad (1b)

Lax representation

The Lax representation

L_t=AL-LA\qquad (2)

of the equation is given by

L=\Sigma \partial_x+\alpha I\partial_y,\qquad (3a)
A= -2i\Sigma\partial_x^2+(-i\Sigma_x-i\alpha\Sigma_y\Sigma+u_yI-\alpha^3u_x\Sigma)\partial_x.\qquad (3b)

Here

\Sigma=\sum_{j=1}^3S_j\sigma_j,\qquad (4)

the \sigma_i are the Pauli matrices and I is the identity matrix.

Reductions

IE 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 IE is the Davey-Stewartson equation.

See also

References

External links

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