“…In the paper [25], it has been shown that for large and stable classes of non-selfadjoint analytic operators in dimension two, the individual eigenvalues can be determined accurately in the semiclassical limit by means of a Bohr-Sommerfeld quantization condition, defined in terms of suitable complex Lagrangian tori close to the real domain. (See also [35] for the formulation of the corresponding Weyl laws.) The work [25] was subsequently continued in a series of papers [12]- [14], [16], [15], all of them concerned with the case of non-selfadjoint perturbations of selfadjoint operators of the form, P ε (x, hD x ) = p w (x, hD x ) + iεq w (x, hD x ), 0 < ε ≪ 1, with the leading symbol p ε (x, ξ) = p(x, ξ) + iεq(x, ξ), (x, ξ) ∈ T * R 2 .…”