cut-off wavelength (original) (raw)

Definition: a wavelength above which a guided mode of a waveguide ceases to exist

Category: article belongs to category fiber optics and waveguides fiber optics and waveguides

Units: m

Formula symbol: ($\lambda_\textrm{co}$)

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DOI: 10.61835/ow7 Cite the article: BibTex plain textHTML Link to this page! LinkedIn

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Contents

Definition of Cut-off Wavelength

The number of guided modes of a waveguide (for example, an optical fiber) depends on the optical wavelength: The shorter the wavelength, the more modes can be guided. For long wavelengths, there may be only a single guided mode (→ single-mode fibers) or even none at all, whereas multimode behavior is obtained at shorter wavelengths.

When a particular mode ceases to exist beyond a certain wavelength, that wavelength is called its cut-off wavelength. For an optical fiber, the cut-off wavelength for the LP11 mode sets a limit to the single-mode regime, as below that wavelength there is at least the LP01 and the LP11 mode.

Modes Close to Cut-off

Just below the cut-off wavelength, the mode properties often vary substantially. Typically, the mode radius (and thus the effective mode area) increases sharply near the cut-off, and the fraction of the optical power propagating within the waveguide core decreases accordingly. That effect is shown in Figure 1 for a multimode step-index fiber; similar behavior occurs for fibers with other transverse refractive index profiles.

fraction of power in fiber core

Figure 1: Fraction of the power of various guided modes (where the colors are related to the ($l$) indices of those) which is contained in the fiber core as a function of the wavelength. The thin vertical lines indicate the calculated cut-off wavelengths of the modes. The diagram has been produced with the software RP Fiber Power.

For LPlm modes of a fiber, only for ($l = 0$) the fraction of the power guided in the core goes to zero when approaching the cut-off. For modes with higher ($l$), the mode size stays finite there, although it may be reduced substantially.

The drastically increased mode size close to cut-off also generally leads to a strong sensitivity to bending (→ bend losses). Even for moderate bending of the fiber one may then obtain sharply increasing propagation losses.

When light from a tunable laser is injected into a fiber, and its wavelength is tuned across the single-mode cut-off, the observed intensity pattern at the fiber's output end shows a sharp transition: It is simply shaped in the single-mode regime, but shows a high sensitivity to the input wavelength and the launch conditions in the multimode regime.

Behavior of Single-mode Fibers at Long Wavelengths

In step-index fibers, there is theoretically no cut-off for the fundamental (LP01) mode, although propagation losses at long wavelengths may still be high, even making the fiber unusable. Even well before running into the spectral region with strong infrared absorption beyond 2 μm wavelength, a single-mode fiber may become unusable for guiding light essentially because long-wavelength light would have a mode size well beyond the fiber core, where the mode becomes very sensitive e.g. to microbending. Note, however, that in such situations there is not a well-defined mode cut-off, but rather one sees gradually rising propagation losses at longer wavelengths.

For other (not step-index) fiber designs, in particular for some photonic crystal fibers, there can also be a fundamental mode cut-off.

Fibers with not radially symmetric designs (and strongly bent fibers) can have polarization-dependent cut-off wavelengths.

RP Fiber Power

Simulations on Cut-off Wavelengths

Explore, for example, how mode properties change near a cut-off wavelength, or what influence the cut-off wavelength of a fiber has on the performance of a device. Only with a suitable simulator, you get complete insight and fully optimize performance. The RP Fiber Power software is an ideal tool for such work.

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