Classical and Quantum Dispersion Relations
arXiv:2003.13559 · doi:10.1088/1402-4896/ab986b
Abstract
It is showed that, in general, classical and quantum dispersion relations are different due to the presence of the Bohm potential. There are exact particular solutions of the quantum (wave) theory which obey the classical dispersion relation, but they differ in the general case. The dispersion relations may also coincide when additional assumptions are made, such as WKB or eikonal approximations, for instance. This general result also holds for non--quantum wave equations derived from classical counterparts, such as in ray and wave optics, for instance. Explicit examples are given for covariant scalar, vectorial and tensorial fields in flat and curved spacetimes.
References in corpus (3)
Cited by in corpus (7)
- Bohm potential is real and its effects are measurable
- Propagation of light in linear and quadratic GRIN media: The Bohm potential
- Quantum particles that behave as free classical particles
- Nondiffracting gravitational waves
- Engineering two-mode squeezed vacuum-like states by using the Bohm potential
- Accelerating Airy tensor modes of cosmological gravitational waves
- On the conditions for the classicality of a quantum particle