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The Photonics Spotlight

Effective Refractive Index: Correcting a Common Belief

Dr. Rüdiger Paschotta

Ref.: encyclopedia articles on effective refractive index

While the refractive index of a homogeneous transparent medium is based on a rather simple concept, the effective refractive index in a waveguide such as an optical fiber is somewhat more difficult to understand – and is in fact often misunderstood.

In a usual single-mode fiber, the guided propagation mode extends significantly beyond the region of the fiber core, and the effective refractive index is found to have a value somewhat between the refractive indices of core and cladding. In a multimode fiber, higher-order modes extend more into the cladding, and have smaller effective indices. These facts often make people believe that the effective index is a kind of weighted average of the local refractive index, according to the propagation of some parts of the total optical power in the core and in the cladding, respectively. This picture, however, is quite wrong.

First consider the definition of the effective index neff: the β value of some fiber mode is neff times the vacuum wavenumber. So that definition targets the phase change per unit length along the fiber axis, not the intensity distribution.

Still one might guess that there is some relation to the intensity distribution as well, but a simple example shows that this can hardly be true. Consider a step-index multimode fiber with high numerical aperture (NA), i.e. with a very large index step. In that case, all fiber modes except for the highest order ones propagate essentially only in the core, so that from this one might expect the effective index of all modes to closely match the core index. But this is not the case: higher-order modes still have significantly lower effective indices. They experience a smaller phase shift per unit length, even though they propagate in the same material. How can that be? Essentially it is the fact that higher-order modes contain more pronounced plane wave components (spatial Fourier components) with a larger angular offset from the fiber axis. So it is here in some sense a matter of different propagation directions, not of different materials. Of course, both effects are relevant in fibers with lower NA.

The figure below shows an example case: a mode of a multimode fiber has been selected, which is close to its cut-off. At this point, the effective refractive index can be calculated to be very close to the cladding index – its difference to the cladding index is only 0.4% of the difference between core and cladding index. The mode field indeed penetrates further into the cladding than other modes, which are not as close to their cut-off. Nevertheless, 68% of the power still propagate within the core.

fiber mode near cut-off

Figure 1: The LP32 mode of a multimode fiber at a wavelength where it is close to its cut-off. The diagram has been produced with the RP Fiber Power software.

One detail can still be confusing: shouldn't modes with stronger off-axis field components experience a larger rather than a smaller phase shift per unit length, given that they somehow have to travel a larger distance? No, that is actually not true: when the k vector has some angle to the fiber axis, its projection to the fiber axis becomes smaller, reducing the phase changes in that direction. This is somewhat reminiscent of a phenomenon discussed in an earlier spotlight article, where that aspect has been discussed in some detail.

This article is a posting of the Photonics Spotlight, authored by Dr. Rüdiger Paschotta. You may link to this page, because its location is permanent. See also the Encyclopedia of Laser Physics and Technology.

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