“…The eigenvalues of P (λ), which we computed with the MATLAB function polyeig, are located in three separate annuli A i , i = 1, 2, 3, given in the first rows of Table 2. These are to be compared to the annuli from the Bini et al generalized Pellet's theorem (see Theorem 3.1), Melman's generalized Pellet's theorem (see [17,Thm. 3.3] or Theorem 3.1 with q k (x) in place of q k (x)), and that of Theorem 2.7 referred to as Pellet 1, Pellet 2, and Tropical, respectively, in Table 2.…”