Abstract
The general equations of a gauge invariant, classical theory of the electrodynamics of material media are obtained. The gauge invariance is insured by taking the equations as conditions auxiliary to the variation principle The Lagrangian function, , depends on D, H, , , and possibly their derivatives; here is the numerical density of atoms in the state , their macroscopic or average velocity, and is a variable that functions as the velocity potential in some cases and has the dimensions of action. The electromagnetic potentials enter the theory as Lagrangian multipliers only.
It is shown that if there is only one state and then the Schrödinger wave equation is obtained on making the substitution
If the atoms are stationary (so that terms in may be neglected), and where is the energy of the state, and is the polarization of the medium, an adequate theory of dispersion results. However, the spontaneous transitions are not correctly accounted for by the equations.
If the electromagnetic fields are neglected and the equations are those for the irrotational motion of a gas, with as the velocity potential.
- Received 9 September 1938
DOI:https://doi.org/10.1103/PhysRev.54.920
©1938 American Physical Society