Logarithmic Schrödinger equation

In theoretical physics, the logarithmic Schrödinger equation (sometimes abbreviated as LNSE or LogSE) is one of the nonlinear modifications of Schrödinger's equation. It is a classical wave equation with applications to extensions of quantum mechanics,[1][2][3] quantum optics,[4] nuclear physics,[5][6] transport and diffusion phenomena,[7][8] open quantum systems and information theory,[9][10][11][12][13][14] effective quantum gravity and physical vacuum models[15][16][17][18] and theory of superfluidity and Bose–Einstein condensation.[19][20] Its relativistic version (with D'Alembertian instead of Laplacian and first-order time derivative) was first proposed by Gerald Rosen.[21] It is an example of an integrable model.

The equationEdit

The logarithmic Schrödinger equation is the partial differential equation. In mathematics and mathematical physics one often uses its dimensionless form:

i{\frac  {\partial \psi }{\partial t}}+\Delta \psi +\psi \ln |\psi |^{2}=0.

for the complex-valued function ψ = ψ(xt) of the particles position vector x = (xyz) at time t, and

{\displaystyle \Delta \psi ={\frac {\partial ^{2}\psi }{\partial x^{2}}}+{\frac {\partial ^{2}\psi }{\partial y^{2}}}+{\frac {\partial ^{2}\psi }{\partial z^{2}}}\,}

is the Laplacian of ψ in Cartesian coordinates. The logarithmic term {\displaystyle \psi \ln |\psi |^{2}} has been shown indispensable in determining the speed of sound scales as the cubic root of pressure for Helium-4 at very low temperatures.[22] In spite of the logarithmic term, it has been shown in the case of central potentials, that even for non-zero angular momentum, the LogSE retains certain symmetries similar to those found in its linear counterpart, making it potentially applicable to atomic and nuclear systems.[23]

The relativistic version of this equation can be obtained by replacing the derivative operator with the D'Alembertian, similarly to the Klein–Gordon equation. Soliton-like solutions known as Gaussons figure prominently as analytical solutions to this equation for a number of cases. 


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