
diameters, so this mode couples very well with a linearly polarized input laser
beam. The flux distribution for the HE
11
mode shown in Fig. 10.8(c) is somewhat
elongated in the direction parallel to the axis of polarization of the mode. Note,
however, that for fibers with larger cores (radius larger than 30a or so), this
asymmetry becomes much less pronounced and the flux distribution becomes
almost azimuthally symmetric. The TE
01
mode is a nondegenerate azimuthally
symmetric mode for which the electric field is always oriented in the azimuthal
direction, as can be seen in Fig. 10.8b. This property, together with the boundary
condition at the interface ...