The Gross-Pitaevskii equation (GPE), a nonlinear Schr ̈odinger equation (NLSE)
for the macroscopic wave functions, governs the properties of a BEC at temperatures
Time dependent Equation is: $ i\hbar\frac{\partial\psi(\bold{x}, t)}{\partial t} = -\frac{\hbar}{2m}\nabla^2\psi(\bold{x}) + \bold{V}(\bold{x}) \psi(\bold{x}) + NU_0 |\psi(\bold{x})|^2\psi(\bold{x}) $
where: $ U_0 = \frac{4\pi\hbar^2a}{m} (a \text{ is scattering length)} $
I've solved this equation numerically by using time-splitting trigonometric spectral approximations of the problem, with periodic boundary conditions.
I've Used time spitting sprectral scheme Lie splitting followed by strang splitting spectral method.
The time-splitting spectral schemes LS and SS are unconditionally
stable. In fact,under any mesh size
The animation of the wave function is shown below.
Simulation of
Potential is
Simulation of
Potential is
Galati, Luigi, "Numerical Solutions to the Gross-Pitaevskii Equation for Bose-Einstein Condensates" (2013). Electronic Theses and Dissertations. 844.