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Nonlinear Schrödinger equation

From Biocrawler, the free encyclopedia.

In theoretical physics, the nonlinear Schrödinger equation is a nonlinear version of Schrödinger's equation in two dimensions. It can be considered as a classical equation, or a second quantized bosonic theory. It is an example of an integrable model.

Classically, we have a complex field ψ satisfying the partial differential equation

i\partial_t\psi=-{1\over 2}\partial^2_x\psi+\kappa|\psi|^2 \psi

It is described by the Hamiltonian

H=\int dx \left[{1\over 2}|\partial_x\psi|^2+{\kappa \over 2}|\psi|^4\right]

with the Poisson brackets

{ψ(x),ψ(y)} = {ψ * (x),ψ * (y)} = 0
* (x),ψ(y)} = iδ(xy)

To get the quantized version, simply replace the Poisson brackets by commutators

[ψ(x),ψ(y)] = [ψ * (x),ψ * (y)] = 0
* (x),ψ(y)] = − δ(xy)

and normal order the Hamiltonian

H=\int dx \left[{1\over 2}\partial_x\psi^\dagger\partial_x\psi+{\kappa \over 2}\psi^\dagger\psi^\dagger\psi\psi\right]

See also

External links

Wikipedia (http://en.wikipedia.org/wiki/Main_Page) Nonlinear_Schrödinger_equation (http://en.wikipedia.org/wiki/Nonlinear_Schrödinger_equation) version history (http://en.wikipedia.org/w/index.php?title=Nonlinear_Schrödinger_equation&action=history) GNU Free Documentation Lizenz (http://en.wikipedia.org/wiki/Wikipedia:Text_of_the_GNU_Free_Documentation_License) CC-by-sa (http://creativecommons.org/licenses/by-sa/2.5/)

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