September 2006
Intermediate to advanced
680 pages
22h 22m
English
book
Ultrashort Laser Pulse Phenomena, 2nd Edition
by Jean-Claude Professor Diels, Jean-Claude Diels, Wolfgang Rudolph
Content preview from Ultrashort Laser Pulse Phenomena, 2nd Edition
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78 Femtosecond Optics
of the device, δ = 2Nπ, and the GVD is:
d
2
d
2
res
=
r + 1
r − 1
d
2
δ
d
2
res
. (2.28)
As is obvious from Eq. (2.19), the second derivative of δ contains the GVD (−k
)
of the material inside the interferometer. This material dispersion is enhanced by
the factor (r + 1)/(r − 1) in condition of resonance. This factor can be large in
the case of a high finesse resonator (1 − r 1).
The GVD given by Eq. (2.27) can be tuned continuously by adjusting δ, which
can be either through a change of the mirror separation d or through a change of
the external angle of incidence . Gires and Tournois [14] conceived this inter-
ferometer to
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