Dielectric Stack Theory

Quarter-wave dielectric stack reflectance. Alternating high/low index layers create high-reflectance mirrors — the basis of dielectric mirrors and VCSELs.

Model: Exact

Peak Reflectance

98.72%

nH/nL Ratio

1.703

Total Layers

10

Stop band (infinite-stack edges)

471–661 nm, width 190 nm

Quarter-Wave Stack Theory

Structure: n₀ | (H L)^N | n_sub

d_H = λ₀/(4n_H),   d_L = λ₀/(4n_L)

R_peak = {[(nH/nL)^(2N) − q] / [(nH/nL)^(2N) + q]}²

q = n₀ / n_sub

Transfer Matrix: M = ∏ M_j,   M_j = [[cos δ, −i sin δ/η], [−i η sin δ, cos δ]]

Model and references

Exact. The equations are exact within the stated assumptions, or are a standard's tabulated values. The results are as good as the inputs. About the tiers

Transfer matrix of an (HL)^N quarter-wave stack at normal incidence with constant, lossless indices; back surface ignored. Peak R at λ₀ and the stop-band edges (of an infinite stack) are closed forms.

  1. Macleod H. A. (2010). Thin-Film Optical Filters, 4th ed., ch. 2 and ch. 6 (quarter-wave stack, high-reflectance zone). CRC Press. doi:10.1201/9781420073034
  2. Born M., Wolf E. (1999). Principles of Optics, 7th ed., §1.6.5 (periodically stratified media). Cambridge University Press.
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