Fundamental lemma (Langlands program): Difference between revisions

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The '''group delay dispersion''' (GDD) of an optical element is the derivative of the [[group delay]] with respect to [[angular frequency]], and also the second derivative of the optical phase. <math>D_2(\omega) = \frac{\partial T_g}{d \omega} = \frac{d^2 \phi}{d\omega^2}</math>. It is a measure of the [[chromatic dispersion]] of the element. A parameter independent of the length of the material is the [[Dispersion (optics)|group velocity dispersion]] (GVD).
 
==Equivalent Parameters==
GDD is related to the total dispersion parameter <math>D</math> as
 
<math> D_2(\omega) = -\frac{2\pi c}{\lambda^2}D_{tot}</math>
 
==References==
[http://www.rp-photonics.com/group_delay_dispersion.html  Encyclopedia of Laser Physics and Technology article on Group Delay Dispersion]
 
[[Category:Optics]]
[[Category:Waves]]
 
 
{{Optics-stub}}

Revision as of 14:31, 18 January 2014

The group delay dispersion (GDD) of an optical element is the derivative of the group delay with respect to angular frequency, and also the second derivative of the optical phase. D2(ω)=Tgdω=d2ϕdω2. It is a measure of the chromatic dispersion of the element. A parameter independent of the length of the material is the group velocity dispersion (GVD).

Equivalent Parameters

GDD is related to the total dispersion parameter D as

D2(ω)=2πcλ2Dtot

References

Encyclopedia of Laser Physics and Technology article on Group Delay Dispersion


Template:Optics-stub