Temporal damping rate, ℑ(f /f_ce), for the branch of Bernstein waves with 2 ⋅ f_ce ≤ f ≤ 3 ⋅ f_ce, presented as a function of the perpendicular (resp. parallel) wave number, k_⊥ (resp. k_||). The wave numbers are normalized relative to the parallel Larmor radius, r_Le,|| = T_th,e,||/ω_ce, and f_pe/f_ce = 1.4. Lines of a constant angle with the magnetic field are also presented. These results were obtained with the numerical linearized Vlasov-Maxwell solver WHAMP, for a homogeneous, magnetized, and Maxwellian plasma (Roennmark 1982).