Lorenz's greatest contribution (1867) is a development of general integral solutions to the differential equations of electromagnetism, which contain retardation effects reflecting the finite speed of light. This paper also introduces the Lorenz gauge, named after him. His 1867 paper can be regarded as contemporaneous with Maxwell's identification of light with electromagnetism waves (1865). 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 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. Lorenz also developed the theory of light propagation through a single homogeneous medium and described the passage of light between different media. The formula for the relationship between the refractive index and the density of a medium was published by Lorenz in 1869 and by
Hendrik Lorentz (who discovered it independently) in 1878 and is therefore called the
Lorentz–Lorenz equation or the Lorenz-Lorentz equation which preserves the historical order. Using his
electromagnetic theory of light he stated what is known as the
Lorenz gauge condition, and was able to derive a correct value for the velocity of light. He also developed a theory of light scattering, publishing it in Danish in 1890 and in French in his Collected Works, published in 1898. It was later independently rediscovered by
Gustav Mie in 1908, so it is sometimes referred to as
Lorenz–Mie theory. Additionally, Lorenz laid the foundations for
ellipsometry by using
Fresnel's theory of
refraction to discover that light reflected at the interface of two media becomes elliptically polarized. ==References==