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Optical Waveguide Modes

Symmetric slab waveguide: V-number, number of TE and TM modes, exact effective indices, core power fraction, b–V diagram and TE mode fields.

Model: Exact

V-number

7.784

(πd/λ)√(n₁² − n₂²); NA = 0.3841

Guided modes

5 TE + 5 TM

⌊2V/π⌋ + 1; single-mode for d < λ/(2NA) = 2.018 µm

TE₀ effective index

1.498429

b = 0.96806; TM₀: 1.498406

TE₀ power in the core

99.63 %

θ_c = 75.16°, acceptance ±22.59° in air

A symmetric slab of thickness d and index n₁ between two claddings of index n₂. With u = V√(1 − b) and w = V√b, TE mode m satisfies u = mπ/2 + arctan(w/u), and TM modes have w multiplied by n₁²/n₂². The page solves these exactly by bisection. Mode m is cut off at V = mπ/2, so the fundamental TE₀ and TM₀ modes are always guided, and the normalized index b = (n_eff² − n₂²)/(n₁² − n₂²) runs from 0 at cutoff towards 1. Here V uses the half-thickness, so it is half the V of Kogelnik and Ramaswamy.

Normalized index b vs V (TE modes)

00.20.40.60.80246810Vb
  • TE0
  • TE1
  • TE2
  • TE3
  • TE4
  • TE5
  • This guide

TE mode fields across the slab

-0.500.51.0-15-10-5051015x (µm), core |x| ≤ d/2E_y (core-normalized)
  • TE0
  • TE1
  • TE2
  • TE3

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

Exact eigenvalue equations of a symmetric step-index slab (TE and TM), solved by bisection. Asymmetric slabs, graded profiles and channel (2D) waveguides are not covered.

  1. Kogelnik H., Ramaswamy V. (1974). Scaling rules for thin-film optical waveguides. Appl. Opt. 13, 1857. doi:10.1364/AO.13.001857
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