In this letter, the kernel of the integral transform that relates the field
quantities over an observation flat plane to the corresponding quantities
on another observation plane parallel to the first one is fractionalized fo
r two-dimensional (2-D) monochromatic wave propagation. It is shown that su
ch fractionalized kernels, with a fractionalization parameter v between zer
o and unity, are the kernels of the integral transforms that provide the fi
eld quantities over the parallel planes between the two original planes. Wi
th a proper choice of the first two planes, these fractional kernels can pr
ovide us with a natural way of interpreting the fields in the intermediate
zones (i.e., the region between the near and far zones) in certain electrom
agnetic problems. The evolution of these fractional kernels into the Fresne
l and Fraunhofer diffraction kernels is addressed. The limit of these fract
ional kernels for the static case is also mentioned. (C) 1999 John Wiley &
Sons, Inc.