The energy levels of fermions bound to the vortex core are considered for t
he general case of chiral superconductors. There are two classes of chiral
superconductivity: in the class I superconducting state the axisymmetric si
ngly quantized vortex has the same energy spectrum of bound states as in an
s-wave superconductor: E = (n 1/2) omega(0), with integral n. In class II
the corresponding spectrum is E = n omega(0) and thus contains a state with
exactly zero energy. The effect of a single impurity on the spectrum of bo
und states is also considered. For class I the spectrum acquires the double
d period Delta E = 2 omega(0) and consists of two equidistant sets of level
s, in accordance with A. I. Larkin and Yu. N. Ovchinnikov, Phys. Rev. B 57,
5457 (1998). For the class II states the spectrum is not influenced by a s
ingle impurity if the same approximation is applied. (C) 1999 American Inst
itute of Physics. [S0021-3640(99)00921-4].