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n - Fachhochschule Jena

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Laser<br />

Principle of Michelson Interferometer<br />

Linearly<br />

polarised<br />

laser mode<br />

Beam<br />

combining<br />

∆φ = (4π/λ0)·(n∆L+L∆n) ·2<br />

Photo<br />

detector<br />

Reflector<br />

Beam<br />

splitting<br />

L 0<br />

Beam splitter Reflector<br />

When does interference<br />

take place?<br />

• Coherence, i.e., defined<br />

phase relations: Path<br />

difference ∆L < coherence<br />

length<br />

L c ~ λ 0 2 /δλ (δλ spectral width)<br />

• Equal states of polarisation<br />

(superposition of electric field<br />

vectors !)<br />

• Almost equal wavelengths<br />

(frequency difference occurs<br />

as intensity modulation<br />

frequency !)<br />

FOS - 39

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