
42 Fundamentals
At given material parameters and carrier frequency, shorter pulses always lead
to a dominant pulse spreading. For T
2
= 10
−10
s (typical value for a single
electronic resonance), and a detuning ωT
2
= 10
4
, we find for example:
τ
rel
W
rel
≈ W
rel
1200 fs
τ
G0
4
. (1.163)
To summarize, a resonant transition of certain spectral width 1/T
2
influences short
pulse (pulse duration < 1ps) propagation outside resonance mainly because of
dispersion. Therefore, the consideration of a transparent material (
i
≈ 0) with
a frequency dependent, real dielectric constant (), which was necessary to
derive Eq. (1.93), is justified in many practical cases involving ...