
The Gross-Pitaevskii equation describes the mean-field dynamics of a Bose-Einstein condensate in terms of a nonlinear Schrödinger equation.In 1961, Eugene Gross and Lev Pitaevskii independently derived the equation that became the main tool of ultracold atomic physics. In a Bose–Einstein condensate, thousands of particles occupy a single quantum state, forming a macroscopic wave. The equation resembles the Schrödinger equation of quantum mechanics, but with an important addition: a term describing the 'friction' of particles against each other (nonlinearity). Thanks to it, quantum vortices—tiny whirlwinds that align themselves into neat lattices—are born in the condensate. By solving the equation, physicists predict such patterns and verify them in experiments with rubidium, sodium, and potassium.
The equation was proposed in 1961 independently by Eugene Gross and Lev Pitaevskii. Gross proceeded from a kinetic approach to superfluidity, Pitaevskii from methods of quantum field theory. Both sought to describe the coherent behavior of many Bose particles. For a long time the work remained a theoretical curiosity, but in 1995, when Eric Cornell, Carl Wieman, and Wolfgang Ketterle first obtained a Bose condensate in a dilute gas (rubidium, sodium), the GP equation instantly became indispensable. Today it serves as the basis for modeling superfluid systems, atom lasers, and quantum simulators.
The equation is solved numerically to calculate the shape and dynamics of a condensate in traps, the interference of two condensates, and the formation of vortex lattices. It is valid for weakly interacting, dilute condensates at temperatures well below the critical temperature (typically nanokelvins). At higher temperatures or stronger interaction, one must account for thermal clouds and three-body losses, which go beyond the mean-field approximation.
It is used to design atom lasers and calculate the properties of superfluid helium—a liquid that can flow without friction through the finest capillaries.
If you 'pinch' a condensate with a focused laser beam, solitons—solitary waves that do not spread out over time—will run along it. It is as if a stone thrown into a pond produced not ripples, but a single hump gliding across the water unchanged.













