A high-n stability code, HINST, has been developed to study the stability o f T AE (Toroidicity induced Alfv en Eigenmodes) in large tokamaks such as ITER where the spectrum of unstable TAE modes is shifted toward medium to high-n modes. The code solves the 2-D eigenmode problem by expanding the eigenfunction in terms of basis functions. Based on the Fourier-ballooning formalism the eigenmode problem is reduced to a system of coupled 1-D equations, which is solved numerically by using the nite element method and a SPARSE matrix solver. The numerical method allows to include non-perturbatively non-ideal eects such as: full ion FLR, trapped electron collisional damping, etc. The 2D numerical results of TAE and Resonance TAE modes are compared with those from local ballooning calculations and global MHD NOVA code. The results show that for ITER-like plasma parameters, TAE and RTAE modes can be driven unstable by alpha particles for n = 1 0 20. The growth rate for the most unstable mode is within the range =! A '0:3 1:5%. The most unstable modes are localized near r=a ' 0:5 and have a broad radial mode envelope width.