For independent electronic transitions, add the electric dipole moment responses:
The positive constants include electron density and transition atomic oscillator strength. Each term adds an absorption peak to and a dispersive positive-to-negative contribution to , as in the middle row of the figure.
Between well-separated absorption lines, where the medium is transparent, the refractive index generally increases with frequency: , or . This is normal dispersion. Near a resonance the real response turns down with increasing frequency, producing an interval of anomalous dispersion, , accompanied by appreciable absorption. The absorptive and dispersive parts are linked by the Kramers-Kronig relations; the steep variation is not independent of the loss spectrum.

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