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Slow Light Structures

Slow light: group delay τ = n_gL/c, group velocity and delay-bandwidth product from a group index, or from a Lorentzian resonance (Brillouin gain, EIT window) whose delay is G/Γ.

Model: Textbook approximation

Group Index n_g

10

slowdown n_g/n₀ = 6.667

Group Velocity c/n_g

29980000 m/s

10 % of c

Group Delay τ

33.36 ps

33.36 ps per mm

Excess Delay over n₀

28.35 ps

background alone: 5.003 ps

Signal Bandwidth Δν

124.8 GHz

Δλ = 1 nm at 1550 nm

Delay × Bandwidth τΔν

4.162

excess Δτ·Δν = 3.538 (≈ bits stored beyond plain propagation)

Model

τ = n_g L/c, v_g = c/n_g, Δν = c/(λ − Δλ/2) − c/(λ + Δλ/2)

τ_res(Δ) = (G/2)·γ(γ² − Δ²)/(γ² + Δ²)², τ_res(0) = G/Γ, γ = Γ/2 = π·FWHM

The group index sets the delay over the structure; the delay-bandwidth product counts how many bits (or pulses) the structure holds at once, which is what limits slow-light buffers. A Lorentzian resonance of power gain G (power e-folds, e^G) has the causal phase (G/2)γΔ/(γ² + Δ²), whose slope is the delay: gain lines and transparency windows slow light, absorption lines (negative gain) speed it up. Its delay times its width is fixed at G/2π, so a narrow line gives long delay over a small bandwidth. Lossless background, one isolated line, signal narrower than the line.

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

τ = n_gL/c and v_g = c/n_g are exact. The resonance is one isolated Lorentzian line with a causal (Kramers–Kronig) phase, a lossless background and a signal narrower than the line; pulse distortion, saturation and the background's own dispersion are not modelled.

  1. Okawachi Y., Bigelow M. S., Sharping J. E. et al. (2005). Tunable all-optical delays via Brillouin slow light in an optical fiber. Phys. Rev. Lett. 94, 153902. doi:10.1103/PhysRevLett.94.153902
  2. Tucker R. S., Ku P.-C., Chang-Hasnain C. J. (2005). Slow-light optical buffers: capabilities and fundamental limitations. J. Lightwave Technol. 23, 4046–4066. doi:10.1109/JLT.2005.853125
  3. Hau L. V., Harris S. E., Dutton Z., Behroozi C. H. (1999). Light speed reduction to 17 metres per second in an ultracold atomic gas. Nature 397, 594–598. doi:10.1038/17561
  4. Baba T. (2008). Slow light in photonic crystals. Nat. Photonics 2, 465–473. doi:10.1038/nphoton.2008.146
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