For a one-dimensional wavefunction,
The probability continuity equation is
For a stationary state , the probability density is independent of time, so and the probability current is constant in space.
For the plane wave
one obtains
This is a momentum eigenstate with momentum and, when it satisfies the free Schrodinger equation, energy . Its constant density and current describe a spatially uniform beam carrying probability in the sign of . It is not a normalizable wavefunction, so it represents an idealized state rather than a localized particle.

Articles by others on the same topic (0)

There are currently no matching articles.