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Home/Optics & Light/Fabry–Pérot Cavity / Etalon

Fabry–Pérot Cavity / Etalon

A Fabry–Pérot cavity consists of two partially reflecting mirrors enclosing a medium of refractive index n and length L. For normal incidence the round-trip phase is δ = 4πnL/λ, and the transmitted intensity follows the Airy function T(δ) = (1−R)²/[(1−R)² + 4R sin²(δ/2)] for symmetric mirror reflectivity R. Sharp resonances appear when δ is a multiple of 2π. The amplitude finesse F = π√R/(1−R) measures how narrow the transmission peaks are; the free spectral range in cavity length is FSR = λ/(2n), and the FWHM linewidth is approximately ΔL ≈ FSR/F. Scanning L (or wavelength) through a resonance is the basis of etalon filters, laser cavities, and high-resolution spectroscopy. This simulator plots T(L), displays F, FSR, and linewidth, and animates a cavity-length scan with a schematic etalon and transmitted beam brightness proportional to T.

Who it's for: Undergraduate optics students after two-beam interference (Michelson/Mach–Zehnder) and before laser cavities or high-finesse spectroscopy.

Key terms

  • Fabry–Pérot etalon
  • Airy function
  • Finesse
  • Free spectral range
  • Linewidth
  • Optical cavity
  • Multiple-beam interference

Live graphs

Fabry–Pérot etalon

633nm
0.95
1
50µm
0.4µm
1×

Symmetric Fabry–Pérot cavity: Airy transmission T = (1−R)²/[(1−R)²+4R sin²(δ/2)] with δ = 4πnL/λ. Finesse F = π√R/(1−R), FSR = λ/(2n), linewidth ΔL ≈ FSR/F.

Measured values

Transmission T12.01%
Finesse F61.2
FSR ΔL316.5 nm
Linewidth ΔL5.2 nm
Order m = 2nL/λ157.98

How it works

Fabry–Pérot etalon: Airy transmission, finesse, free spectral range, and linewidth as you scan cavity length L.

Key equations

T(δ) = (1−R)² / [(1−R)² + 4R sin²(δ/2)]
δ = 4πnL/λ · F = π√R/(1−R) · FSR = λ/(2n) · ΔL ≈ FSR/F

Frequently asked questions

What is finesse?
Finesse F = π√R/(1−R) quantifies how many sharp transmission peaks fit within one free spectral range. Higher R (and higher F) gives narrower resonances.
What is the free spectral range?
FSR = λ/(2n) is the cavity-length spacing between adjacent transmission peaks at fixed wavelength. In frequency, FSR = c/(2nL).
How is linewidth related to finesse?
Approximately ΔL ≈ FSR/F. High-finesse cavities transmit only a very narrow range of lengths or wavelengths near resonance.
What is left out?
Mirror absorption, surface figure, walk-off at angle, thermal drift, and frequency-dependent dispersion in the medium are not modeled.