Resistive magnetohydrodynamic spectra of toroidal plasmas are calculated us
ing the recently developed Jacobi-Davidson eigenvalue solver. Poloidal mode
coupling in finite aspect ratio tokamaks yields gaps in the ideal Alfven c
ontinuous spectrum. If resistivity is included, the ideal continua disappea
r and are replaced by damped global waves located on specific curves in the
complex frequency plane. The end points of these curves join the tips of t
he ideal continua and the boundaries of the ideal spectral gap. The eigenfu
nctions of the waves on these resistive curves are shown to have definite p
arity in the poloidal harmonics. It is shown that for very small toroidicit
y the topology of the resistive spectrum is completely different from the c
ylindrical one. Independent of the size of the inverse aspect ratio the ide
al gap remains visible in the resistive spectrum. (C) 1999 American Institu
te of Physics. [S1070-664X(99)01805-4].