The Lorenz gauge condition is used to eliminate the redundant spin-0 component in Maxwell's equations when these are used to describe a massless spin-1 quantum field. It is also used for massive spin-1 fields where the concept of gauge transformations does not apply at all.
A quick justification of the Lorenz gauge can be found using
Maxwell's equations and the relation between the magnetic vector potential and the magnetic field:
Therefore,
Since the curl is zero, that means there is a scalar function such that
This gives a well known equation for the electric field:
To have Lorentz invariance, the time derivatives and spatial derivatives must be treated equally (i.e. of the same order). Therefore, it is convenient to choose the Lorenz gauge condition, which makes the left hand side zero and gives the result
A similar procedure with a focus on the electric scalar potential and making the same gauge choice will yield
These are simpler and more symmetric forms of the inhomogeneous
Maxwell's equations.
Here
is the vacuum velocity of light, and is the
d'Alembertian operator. These equations are not only valid under vacuum conditions, but also in polarized media,[7] if and are source density and circulation density, respectively, of the electromagnetic induction fields and calculated as usual from and by the equations
The explicit solutions for and – unique, if all quantities vanish sufficiently fast at infinity – are known as
retarded potentials.
History
When originally published in 1867, Lorenz's work was not received well by
James Clerk Maxwell. Maxwell had eliminated the
Coulomb electrostatic force from his derivation of the
electromagnetic wave equation since he was working in what would nowadays be termed the
Coulomb gauge. The Lorenz gauge hence contradicted Maxwell's original derivation of the EM wave equation by introducing a retardation effect to the Coulomb force and bringing it inside the EM wave equation alongside the time varying
electric field, which was introduced in Lorenz's paper "On the identity of the vibrations of light with electrical currents". Lorenz's work was the first use of
symmetry to simplify Maxwell's equations after Maxwell himself published his 1865 paper. In 1888, retarded potentials came into general use after
Heinrich Rudolf Hertz's experiments on
electromagnetic waves. In 1895, a further boost to the theory of retarded potentials came after
J. J. Thomson's interpretation of data for
electrons (after which investigation into
electrical phenomena changed from time-dependent
electric charge and
electric current distributions over to moving
point charges).[2]
^For example, see Cheremisin, M. V.; Okun, L. B. (2003). "Riemann-Silberstein representation of the complete Maxwell equations set".
arXiv:hep-th/0310036.