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Cavity Mode Spacing and Stability

Two-mirror resonator: g-parameters and stability diagram, free spectral range, transverse mode spacing, TEM₀₀ waist size and position, and spot sizes on the mirrors.

Model: Textbook approximation

g₁ / g₂

-0.5000 / -0.5000

g = 1 − L/R

g₁g₂

0.2500

Stable

Free spectral range c/(2nL)

0.9993 GHz

8.008 pm at λ

Transverse mode spacing

0.6662 GHz

One-way Gouy phase θ = 120.0°

Waist radius w₀ (1/e²)

146.2 µm

Rayleigh range 43.30 mm in the medium

Waist distance from mirror 1

75.00 mm

Towards mirror 2; negative is behind mirror 1

Spot radius on mirror 1

292.3 µm

Spot radius on mirror 2

292.3 µm

g₁ = 1 − L/R₁, g₂ = 1 − L/R₂; stable for 0 ≤ g₁g₂ ≤ 1. νqmn= FSR [q + (m + n + 1) θ/π], θ = arccos(±√(g₁g₂)), + for g > 0 and − for g < 0.

zR² = L² g₁g₂(1 − g₁g₂)/(g₁ + g₂ − 2g₁g₂)², w₀² = λzR/(nπ), z₁ = L g₂(1 − g₁)/(g₁ + g₂ − 2g₁g₂), w₁² = (λL/nπ)√(g₂/(g₁(1 − g₁g₂))).

For a dispersive filling the mode spacing uses the group index: FSR = c/(2ngL); the index input here is the phase index.

Mode frequencies relative to TEM₀₀ of order q (stick height marks the order, not the power)

00.20.40.60.81.000.51.01.5ν − ν(q, 00) (GHz)Transverse order (taller = lower)
  • m + n = 0
  • m + n = 1
  • m + n = 2
  • m + n = 3
  • m + n = 4

Stability diagram: stable between the axes and the hyperbola

-202-3-2-10123g₁g₂
  • g₁g₂ = 1 (boundary)
  • g₁g₂ = 1, negative branch
  • g₁ = 0 and g₂ = 0 (boundary)
  • Symmetric: planar, confocal, concentric
  • This cavity

Model and references

Textbook approximation. A standard approximation from the literature (for example paraxial, plane-wave or Gaussian-beam), valid within the range the page states. About the tiers

Paraxial Gaussian modes of two spherical mirrors (Kogelnik–Li), with a medium of index n filling the cavity (phase index; a dispersive filling spaces the modes by c/(2n_gL)). The transverse spacing takes the Gouy phase on the branch set by the sign of g, so cavities with g < 0 space their modes by more than FSR/2. Aperture losses and mirror tilt are ignored.

  1. Kogelnik H., Li T. (1966). Laser beams and resonators. Appl. Opt. 5, 1550–1567. doi:10.1364/ao.5.001550
  2. Siegman A. E. (1986). Lasers, ch. 19. University Science Books.
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