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Figure 7.4 The solid line shows the real part of (7.122), and the dotted line, the imaginary part. All parameters are in units of the shifted resonance of the medium wb given by (7.123). We used a' = wb and K = O.lwb. This complex dielectric permittivity exhibits all the typical features we expect. There is an region of anomalous dispersion near the resonance of the medium, where the refractive index decreases with frequency rather than increasing. For large frequencies, the real part of e tends to 1, making the refractive index of the medium the same as that of the vacuum.

Huttner and Barnett's approach consists in finding the set of annihilation and creation operators that diagonalizes the total Hamiltonian (7.96), then expressing the electro-

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magnetic field operators in terms of them. This way they were able to develop a fully Canonical quantum theory of electrodynamics in a linear dielectric, including dispersion and absorption. The diagonalization is done using a technique developed by Fano [190] in 1961, which they adapted to deal directly with operators rather than wavefunctions [38]. First, H mat is diagonalized, then the rest of the Hamiltonian. We will follow their approach with a few technical changes required by our simplifying assumptions of small losses and white noise. These assumptions not only make the discussion more pedagogical, but also allow us to calculate explicitly things for which they could only derive formal expressions. One of these things is the permittivity. In their general approach, Huttner and Barnett have interpreted a certain function as the dielectric permittivity. They have not shown that it is the permittivity that one finds in the classical theory. Here we will be able to calculate this function and show that it coincides lO with (7.122).

To obtain tractable expressions, we will use our small coupling, white noise assumption with Wo 6. ,... These assumptions will allow us to extend integrals over 1] to -<Xl, taking V(1]) as constant and equal to V == V(wo) = ,../1f. Let us define the dressed operator

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