We study the r modes and rotational "hybrid" modes (inertial modes) of rela
tivistic stars. As in Newtonian gravity, the spectrum of low-frequency rota
tional modes is highly sensitive to the stellar equation of state. If the s
tar and its perturbations obey the same one-parameter equation of state (as
with barotropic stars), there exist no pure r modes at all-no modes whose
limit, for a star with zero angular velocity, is an axial-parity perturbati
on. Rotating stars of this kind similarly have no pure g modes, no modes wh
ose spherical limit is a perturbation with polar parity and vanishing pertu
rbed pressure and density. In spherical stars of this kind, the r modes and
g modes form a degenerate zero-frequency subspace. We find that rotation s
plits the degeneracy to zeroth order in the star's angular velocity Omega,
and the resulting modes are generically hybrids, whose limit as Omega -->0
is a stationary current with both axial and polar parts. Because each mode
has definite parity, its axial and polar parts have alternating values of l
. We show that each mode belongs to one of two classes, axial-led or polar-
led, depending on whether the spherical harmonic with the lowest value of I
that contributes to its velocity field is axial or polar. Newtonian barotr
opic stars retain a vestigial set of purely axial modes (those with l=m); h
owever, for relativistic barotropic stars, we show that these modes must al
so be replaced by axial-led hybrids. We compute the post-Newtonian correcti
ons to the l=m modes for uniform density stars. On the other hand, if the s
tar is nonbarotropic (that is, if the perturbed star obeys an equation of s
tate that differs from that of the unperturbed star), the r modes alone spa
n the degenerate zero-frequency subspace of the spherical star. In Newtonia
n stars, this degeneracy is split only by the order-Omega (2) rotational co
rrections. However, when relativistic effects are included, the degeneracy
is again broken at zeroth order. We compute the I modes of a nonbarotropic,
uniform density model to first post-Newtonian order.