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INTERFEROMETER
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Fabry Pérot Interferometer
Maurice Paul Auguste Charles Fabry ( ) Alfred Pérot ( )
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Michelson Fringes Fabry Perot Fringes
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Fabry-Perot Interferometer
S2 S1
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T+R+A=1 T: Transmittance (tt) R : Reflectance (r2) A: Absorbance
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Irradiance d: successive phase difference of the transmitted rays
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A A (q) : Airy’s function A
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Measurement of sharpness of fringes
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Finesse F of the mirror system is defined by
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Chromatic Resolving power
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Fabry-Perot Interferometer
θ o 30
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I0
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IR/I IT/I φ
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Transmitted intensity
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d/λ = 10 , f = 8 d/λ = 10 , f = 1 θ θ d/λ = 1000 , f = 7
o θ 30 θ d/λ = 1000 , f = 7 d/λ = 10 , f = 2 θ θ o 3
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Michelson fringes Fabry-Perot fringes
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Full width at half maximum
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Resolved wavelengths
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Unresolved wavelengths
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Barely resolved
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Chromatic resolving power of
Fabry Perot interferometer
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Doublet separation in Fabry-Perot interferometer
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&
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λ1= 589.0 nm λ2= 589.6 nm Δλ= 0.6 nm λ/Δλ~1000 CRP<1000
Sodium doublet λ1= nm λ2= nm Δλ= 0.6 nm λ/Δλ~1000 CRP<1000
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λ1= 589.0 nm λ2= 589.6 nm Δλ= 0.6 nm λ/Δλ~1000 CRP ~ 1000
Sodium doublet λ1= nm λ2= nm Δλ= 0.6 nm λ/Δλ~1000 CRP ~ 1000
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λ1= 589.0 nm λ2= 589.6 nm Δλ= 0.6 nm λ/Δλ~1000 CRP >1000
Sodium doublet λ1= nm λ2= nm Δλ= 0.6 nm λ/Δλ~1000 CRP >1000
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λ1= 589.0 nm λ2= 589.6 nm Δλ= 0.6 nm λ/Δλ~1000 CRP >> 1000
Sodium doublet λ1= nm λ2= nm Δλ= 0.6 nm λ/Δλ~1000 CRP >> 1000
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λ1= 589.0 nm λ2= 589.6 nm Δλ= 0.6 nm λ/Δλ~1000 CRP>>>1000
Sodium doublet λ1= nm λ2= nm Δλ= 0.6 nm λ/Δλ~1000 CRP>>>1000
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