Eckhaus equation

In mathematical physics, the Eckhaus equation, a nonlinear partial differential equations within the nonlinear Schrödinger class:

$i\psi _{t}+\psi _{xx}+2\left(|\psi |^{2}\right)_{x}\,\psi +|\psi |^{4}\,\psi =0.$

was introduced by Wiktor Eckhaus to model the propagation of waves in dispersive media.. A generalization of this equation with additiobal cubic nonlinear term was proposed earlier by Anjan Kundu through gauge equivalence from the nonlinear Schrödinger equation, which is now known as the Kundu-Eckhaus equation.

Linearization

Animation of a wave-packet solution of the Eckhaus equation. The blue line is the real part of the solution, the red line is the imaginary part and the black line is the wave envelope (absolute value). Note the asymmetry in the envelope $|\psi (x,t)|$ for the Eckhaus equation, while the envelope $|\varphi (x,t)|$ – of the corresponding solution to the linear Schrödinger equation – is symmetric (in $x$). The short waves in the packet propagate faster than the long waves.

Animation of the wave-packet solution of the linear Schrödinger equation – corresponding with the above animation for the Eckhaus equation. The blue line is the real part of the solution, the red line is the imaginary part, the black line is the wave envelope (absolute value) and the green line is the centre of gravity of the wave packet.

The Eckhaus equation can be linearized to the linear Schrödinger equation:

$i\varphi _{t}+\varphi _{xx}=0,$

through the non-linear transformation:

$\varphi (x,t)=\psi (x,t)\,\exp \left(\int _{-\infty }^{x}|\psi (x^{\prime },t)|^{2}\;{\text{d}}x^{\prime }\right).$

The inverse transformation is:

$\psi (x,t)={\frac {\varphi (x,t)}{\displaystyle \left(1+2\,\int _{-\infty }^{x}|\varphi (x^{\prime },t)|^{2}\;{\text{d}}x^{\prime }\right)^{1/2}}}.$

This linearization also implies that the Eckhaus equation is integrable.

References

• Ablowitz, M.J.; Ahrens, C.D.; De Lillo, S. (2005), "On a "quasi" integrable discrete Eckhaus equation", Journal of Nonlinear Mathematical Physics, 12 (Supplement 1): 1–12, Bibcode:2005JNMP...12S...1A, doi:10.2991/jnmp.2005.12.s1.1
• Calogero, F.; De Lillo, S. (1987), "The Eckhaus PDE iψ_t + ψ_xx+ 2(|ψ|²)_x ψ + |ψ|⁴ ψ = 0", Inverse Problems, 3 (4): 633–682, Bibcode:1987InvPr...3..633C, doi:10.1088/0266-5611/3/4/012
• Eckhaus, W. (1985), The long-time behaviour for perturbed wave-equations and related problems, Department of Mathematics, University of Utrecht, Preprint no. 404.
  Published in part in: Eckhaus, W. (1986), "The long-time behaviour for perturbed wave-equations and related problems", in Kröner, E.; Kirchgässner, K. (eds.), Trends in applications of pure mathematics to mechanics, Lecture Notes in Physics, vol. 249, Berlin: Springer, pp. 168–194, doi:10.1007/BFb0016391, ISBN 978-3-540-16467-8
• Kundu, A. (1984), "Landau–Lifshitz and higher-order nonlinear systems gauge generated from nonlinear Schrödinger-type equations", Journal of Mathematical Physics, 25: 3433–3438, Bibcode:1984JMP....25.3433K, doi:10.1063/1.526113
• Taghizadeh, N.; Mirzazadeh, M.; Tascan, F. (2012), "The first-integral method applied to the Eckhaus equation", Applied Mathematics Letters, 25 (5): 798–802, doi:10.1016/j.aml.2011.10.021
• Zwillinger, D. (1998), Handbook of differential equations (3rd ed.), Academic Press, ISBN 978 0 12 784396 4