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Eckhaus equation : ウィキペディア英語版
Eckhaus equation
In mathematical physics, the Eckhaus equation – or the Kundu–Eckhaus equation – is a nonlinear partial differential equations within the nonlinear Schrödinger class:
:i \psi_t + \psi_ +2 \left( |\psi|^2 \right)_x\, \psi + |\psi|^4\, \psi = 0.
The equation was independently introduced by Wiktor Eckhaus and by Anjan Kundu to model the propagation of waves in dispersive media.
==Linearization==

The Eckhaus equation can be linearized to the linear Schrödinger equation:
:i \varphi_t + \varphi_ =0,
through the non-linear transformation:
:\varphi(x,t) = \psi(x,t)\, \exp\left( \int_^x |\psi(x^\prime,t)|^2\; \textx^\prime \right).
The inverse transformation is:
:\psi(x,t) = \fracx^\prime \right)^}.
This linearization also implies that the Eckhaus equation is integrable.

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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