Mixtures of coherent and thermal fields

When I started my PhD, there arose the need to describe mixtures of coherent and thermal states, specifically the diagonal elements $p(n)$ of the density matrix (or probability to have $n$ particles) and the postdoc there came up with something that looked hideous to me: $p_{\mathrm{coh}}(n)+p_{\mathrm{th}}(n)$ (normalized).

I was stuyding Glauber's $P$ function formalism then, where it was stated how to admix various fields from their $P$ function. Strangely enough, the statistics $p(n)$ for a mixture of coherent and thermal fields were not worked out, so I did it myself and we used this version instead for the paper.[1]

Of course, such a basic result had been derived before. Apparently the first time by G. Lachs[2]. One can also find the result in Teich and Saleh's excellent book Fundamentals of Photonics.

Possibly also related B. Picinbono and M. Rousseau, Phys. Rev. A 1:635 (1970).

References

  1. Effects of Bose-Einstein condensation of exciton polaritons in microcavities on the polarization of emitted light. F. P. Laussy, I. A. Shelykh, G. Malpuech and A. Kavokin in Phys. Rev. B 73:035315 (2006). Pdf-48px.png
  2. Template:Lachs65a