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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122 Femtosecond Optics
Table 2.2
Values of second-order dispersion for typical devices.
Device λ
(nm) ω
(fs
−1
)
(fs
2
)
Fused silica (L
g
= 1 cm) 620 3.04 535
800 2.36 356
Brewster prism 620 3.04 −760
pair, fused silica
L = 50 cm 800 2.36 −523
Grating pair 620 3.04 −9.3 ×10
4
b = 20 cm; β = 0
◦
d = 1.2 µm 800 2.36 −3 ×10
5
The choice between gratings and prism for controllable dispersion is not
always a simple one. Prisms pairs have lower losses than gratings (the total trans-
mission through a grating pair usually does not exceed 80%), and are therefore
the preferred intracavity dispersive element. Gratings are often used in amplifier
chain where extremely high ...
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