Equivalence of the Langevin and auxiliary-field quantization methods for absorbing dielectrics

Recently two methods have been developed for the quantization of the electromagnetic field in general dispersing and absorbing linear dielectrics. The first is based upon the introduction of a quantum Langevin current in Maxwell's equations [T. Gruner and D.-G. Welsch Phys. Rev. A 53, 1818 (1996), Ho Trung Dung, L. Knoll, and D.-C. Welsch, Phys. Rev. A 57, 3931 (1998); S. Scheel, L. Knell, and D.-G. Welsch, Phys. Rev. A 58, 700 (1998)], whereas the second makes use of a set of auxiliary fields, followed by a canonical quantization procedure [A. Tip, Phys. Rev. A 57, 4818 (1995)]. We show that both approaches are equivalent.