The Hamiltonian acting on this quantity equals an energy eigenvalue multiplied by this quantity in the time-independent Schrödinger equation.
BoseÂ–Einstein condensates can be described by a macroscopic version of this quantity equal to the root of the density distribution times a spatially varying phase factor. The anti-symmetrizer of this quantity can yield a determinant of many of these quantities. This quantity is assumed to be exponential with a slowly varying phase and amplitude compared to the de Broglie (de BROY-yeh) wavelength in the WÂ·KÂ·B approximation. The squared magnitude of this quantity gives the probability density, which is normalized to one when integrated. The Hamiltonian acting on this quantity equals an energy eigenvalue multiplied by this quantity in the time-independent Schrödinger equation. For 10 points, name this quantity, symbolized psi ("sigh"), that describes the quantum state of a particle.
BoseÂ–Einstein condensates can be described by a macroscopic version of this quantity equal to the root of the density distribution times a spatially varying phase factor.
wavefunctions