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
It is described by the Hamiltonian
with the Poisson brackets
- {ψ(x),ψ(y)} = {ψ * (x),ψ * (y)} = 0
- {ψ * (x),ψ(y)} = iδ(x − y)
To get the quantized version, simply replace the Poisson brackets by commutators
- [ψ(x),ψ(y)] = [ψ * (x),ψ * (y)] = 0
- [ψ * (x),ψ(y)] = − δ(x − y)
and normal order the Hamiltonian
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See also
- Phi to the fourth for a related model in quantum field theory.
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External links
- Nonlinear Schrodinger Equation with a Cubic Nonlinearity (http://eqworld.ipmnet.ru/en/solutions/npde/npde1401.pdf) at EqWorld: The World of Mathematical Equations.
- Nonlinear Schrodinger Equation with a Power-Law Nonlinearity (http://eqworld.ipmnet.ru/en/solutions/npde/npde1402.pdf) at EqWorld: The World of Mathematical Equations.
- Nonlinear Schrodinger Equation of General Form (http://eqworld.ipmnet.ru/en/solutions/npde/npde1403.pdf) at EqWorld: The World of Mathematical Equations.

