Although their mathematical forms apparently resemble each other, the
diffraction integral and fractional Fourier transformation (FRT) have
completely different physical meanings. We point out that an interpret
ation of the FRT given recently in a paper by Alieva et al, is not phy
sically appropriate. We then show how those integral transformations c
an be treated in a unified way within the framework of the special aff
ine Fourier transformation. Finally the multidimensional FRT presented
in the above paper is further generalized to allow n independent frac
tional degrees.