Effective Mode Area
Modes of fibers or other waveguides have smooth transverse profiles where the definition of a mode area is not straightforward, particularly for complicated mode shapes where e.g. some 1/e2 intensity criterion as for Gaussian beams is not sensible. A useful definition for the effective mode area is
where E is the electric field amplitude and I is the optical intensity. The integration is done not only over the core area, but over the whole plane. For a Gaussian beam with radius w, the effective area is π w2, and the same equation is valid for relating the mode area to the effective mode radius. The equation would also hold for a rectangular (flat-top) intensity profile with radius w.
Figure 1 shows a Gaussian mode and a rectangular profile with the same effective mode area. For the same optical power, the Gaussian mode has twice the peak intensity.
where P is the optical power and L is the length of the medium. It is assumed that the nonlinear index is constant over the whole area, which is not accurate for all fibers, as the index-raising dopants can also influence the nonlinearity. Note that the nonlinear phase shift applies to the whole mode area, rather than e.g. only to the point with highest intensity, as the waveguide effect prevents the build-up of any significant transverse variations of the optical phase.
Note that depending on the shape of the mode profile, the effective area may deviate substantially from π w2 where the radius w is calculated either as an 1/e2 intensity value or with the D4σ method. In most practical cases, however, these deviations are not very large.
Typical single-mode fibers, as used e.g. for optical fiber communications, have effective mode areas of the order of 100 μm2. Large mode area fibers have several times higher mode areas, sometimes even above 1000 μm2. On the other hand, there are highly nonlinear fibers with particularly small mode areas. Some photonic crystal fibers can have mode areas below 10 μm2.
An important consequence of a small mode area is that the optical intensities for a given power level are high, so that nonlinearities become important. Also, small mode areas are usually the consequence of strong guiding, where bend losses and other effects of external disturbances are weak.
If two fibers with different effective mode areas are spliced together, this will lead to some optical power loss. The article on fiber joints contains a formula for estimating that coupling loss. For efficiently coupling fibers with substantially different mode areas, certain mode field converters (or mode area adapters) are sometimes used. Often, these are made from tapered fibers, adiabatically expanding or compressing the fiber modes.
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