cut-off wavelength (original) (raw)

Author: the photonics expert

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: <$\lambda_\textrm{co}$>

DOI: 10.61835/ow7 [Cite the article](encyclopedia%5Fcite.html?article=cut-off wavelength&doi=10.61835/ow7): BibTex plain textHTML Link to this page share on LinkedIn

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.

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 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.

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. This is essentially because long-wavelength light would have a mode size well beyond the fiber core, with such mode experiencing light guidance and thus being 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.

Just below its cut-off wavelength, the bend losses of a mode can become very high due to the increased mode area. Therefore, even for moderate bending of the fiber one may obtain sharply increasing propagation losses near the cut-off wavelength. Therefore, cut-off wavelengths can not always be precisely determined in experiments.

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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