A review of the present theoretical understanding of the linear stabil
ity of internal m = 1 modes is presented and its connection to phenome
na observed in toroidal magnetic confinement experiments, i.e. 'sawtoo
th' and 'fishbone' oscillations, is discussed. Particular attention is
devoted to the analysis of nonmagnetohydrodynamic (non-MHD) effects,
such as those due to finite diamagnetic and electron drift frequencies
and to finite ion Larmor radius, and to the special role played by en
ergetic particles (whose response is primarily kinetic and which can s
tabilize low frequency modes and destabilize new, higher frequency, br
anches). Some recent developments in the non-linear theory of these mo
des are also discussed. This review complements that of Kuvshinov and
Savrukhin (Sov. J. Plasma Phys. 16 (1990) 353).