Acousto optical modulators


by Niles
Tags: acousto, modulators, optical
Niles
Niles is offline
#1
Feb9-12, 03:24 PM
P: 1,863
Hi

Say I am looking at an AOM working in the Bragg regime (i.e., only a single diffracted beam). It is easy to show using Bragg's law that the frequency-shift Ω of the diffracted wave is given by
[tex]
\Omega = 2n\omega \frac{v}{c}\sin(\theta)
[/tex]
Here Ω is *also* the frequency the AOM is driven with, in other words the LHS is constant in the sense that in does not depend on the incoming light (so the frequency-shift imparted on the wave is constant). However, the RHS does depend on the incoming light, since the angle θ of the diffracted beam is equal to the angle of incidence of the incoming beam, so I can change it easily by e.g. turning the AOM.

In my book it says that the shift Ω is zero for forward scattering and maximum for backscattering. This is what I don't understand: The shift Ω is the same as the frequency of the phonons in the material, which is *constant*. So how can I change the frequency shift of the diffracted wave by changing the angle on incidence?

Best,
Niles.
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Niles
Niles is offline
#2
Feb10-12, 02:47 AM
P: 1,863
OK, I understand my error now.
Andy Resnick
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#3
Feb10-12, 07:18 AM
Sci Advisor
P: 5,468
What book are you using? I have one by Korpel, and it's not working for me...

Niles
Niles is offline
#4
Feb10-12, 01:05 PM
P: 1,863

Acousto optical modulators


I am using Boyd's Nonlinear Optics, it has a nice chapter on spontaneous light-scattering including Acoustooptics. I hope it works out.

Best,
Niles.


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