Dielectric High Reflector

Quarter-wave dielectric stack HR mirror — stopband width, peak reflectance, and dispersion.

Model: Exact

Reflectance at λ₀

99.9930 %

1 − R = 7.04e-5

Stop band (R ≥ 50 %)

372 nm

909.7 nm – 1281.4 nm

Group delay at λ₀

1.972 fs

Semi-infinite stack: 1.972 fs; GDD(λ₀) = 0

Zone of the infinite stack: 923.4 nm – 1255.0 nm (332 nm, Δg = 0.1522)

Layers: 21; dH = 113.2 nm, dL = 183.4 nm

R(λ₀) = ((n₀ − Y)/(n₀ + Y))², each quarter-wave layer mapping the admittance Y → n²/Y from Y = ns. The stop band is the actual stack's, from λ₀ out to the first 50 % points (side lobes excluded); the zone λ₀/(1 ± Δg), Δg = (2/π) asin((nH − nL)/(nH + nL)), is the limit of many pairs. Group delay τ = d(arg r)/dω and GDD = d²(arg r)/dω² on reflection, front face as reference. At λ₀ the semi-infinite stack gives τ = λ₀n₀/(2cΔn) with H outermost and λ₀nHnL/(2cn₀Δn) with L outermost.

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 (HL)^N H or (LH)^N quarter-wave stacks, normal incidence, constant lossless indices, back surface ignored. Group delay and GDD are central differences of arg r.

  1. Macleod H. A. (2010). Thin-Film Optical Filters, 4th ed., ch. 2 and ch. 6 (multilayer high-reflectance coatings). 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.
  3. Babic D. I., Corzine S. W. (1992). Analytic expressions for the reflection delay, penetration depth, and absorptance of quarter-wave dielectric mirrors. IEEE J. Quantum Electron. 28, 514. doi:10.1109/3.123281
Report a problem

A wrong value, a formula, a reference, or a page that misbehaves. The report includes this page and its current inputs.