In this letter, we demonstrate the existence of unstable ion temperature gr
adient driven Alfven eigenmodes in tokamak plasmas, which are ideally stabl
e with respect to magnetohydrodynamics (MHD). Conditions for the destabiliz
ation of such modes are quantitatively discussed on the basis of theoretica
l analyses of the mode dispersion relation, which is given in a compact ana
lytical form. It is emphasized that instability requires both sufficiently
strong thermal ion temperature gradients and that the plasma be sufficientl
y close to ideal MHD marginal stability.