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Mode Matching

The single lens, and its position, that couples one Gaussian beam waist into another, plus the best coupling of a lens you already have.

Model: Textbook approximation

Matching lens focal length f

36.22 mm

The one positive lens that couples 100 %

Lens distance from input waist s₁

43.72 mm

Lens distance to target waist s₂

156.3 mm

Shortest usable focal length f₀ = πw₁w₂/λ

20.27 mm

Magnification w₂/w₁

4.000

Rayleigh ranges z_R1 / z_R2

5.067 / 81.07 mm

Your lens: best distance from input waist

49.28 mm

Your lens: coupling η

97.67 %

Best over positions between the waists

f₀ = πw₁w₂/λ; for f ≥ f₀: s₁ = f ± (w₁/w₂)√(f² − f₀²), s₂ = f ± (w₂/w₁)√(f² − f₀²), s₁ + s₂ = d.

Coupling of beams q₁, q₂ at one plane (q = z + izR): η = 4 Im q₁ Im q₂ / |q₁ − q₂*|², which includes both the size and the wavefront curvature mismatch.

Best coupling versus lens focal length

2040608010020406080100120140Focal length f (mm)Coupling η (%)
  • Best η at each focal length
  • Matching lens (η = 100 %)
  • Your lens

Beam radius along the axis

100200300400500050100150200Distance from the input waist z (mm)Beam radius w (µm)
  • Matching lens
  • Your lens at its best position
  • Target beam

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 TEM₀₀ beams and a thin lens, closed-form solution. Coupling η is the exact overlap of the two Gaussian beams, including wavefront curvature; aberrations, tilt and lateral offset are ignored.

  1. Kogelnik H., Li T. (1966). Laser beams and resonators. Appl. Opt. 5, 1550–1567. doi:10.1364/ao.5.001550
  2. Self S. A. (1983). Focusing of spherical Gaussian beams. Appl. Opt. 22, 658. doi:10.1364/ao.22.000658
  3. Joyce W. B., DeLoach B. C. (1984). Alignment of Gaussian beams. Appl. Opt. 23, 4187. doi:10.1364/ao.23.004187
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