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Brillouin-Light-Scattering Spectroscopy

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Linear<br />

relation:<br />

Δν<br />

( Δl)<br />

= ν<br />

R<br />

Fabry-Pérot interferometer<br />

−ν<br />

=<br />

c<br />

λ<br />

Maximal transmission:<br />

R<br />

⎛<br />

⎜<br />

⎜ 1<br />

1−<br />

⎜ Δl<br />

⎜ 1+<br />

⎝ lR<br />

Benjamin Jungfleisch SFB/TR49 Student Seminar 20th to 21th of July 2010<br />

⎞<br />

⎟<br />

⎟<br />

⎟<br />

⎟<br />

⎠<br />

=<br />

c<br />

λ<br />

R<br />

l<br />

R<br />

l =<br />

Δl<br />

+ Δl<br />

m<br />

optical bandpass<br />

freuquency measurement<br />

⎛ Δl<br />

⎞<br />

λ(<br />

Δl)<br />

= λ ⎜ + ⎟<br />

R 1<br />

⎝ lR<br />

⎠<br />

≈<br />

λ<br />

2<br />

c<br />

λ<br />

R<br />

Δl<br />

l<br />

for lR= 0,3 mm: Δν= 500 GHz<br />

R

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