We make two remarks about the calculation of the large imaginary component
of the quasinormal modes associated with a Schwarzschild black hole. First,
we display an analytical approximation for the radial component of the Reg
ge-Wheeler-Zerilli equation that yields, to the lowest order, the main asym
ptotic value for the imaginary part of these quasinormal modes. The link be
tween the boundary conditions and the value adopted by the quasinormal freq
uency is transparent within this approximation. In a second part, we refer
to the strategy followed by Nollert in his search of these modes. The quasi
normal modes appear as the frequencies that avoid the divergence of a conti
nued fraction. The terms from n = N to infinity, in this series, are replac
ed for what is called the remainder R-N(omega). In searching these frequenc
ies, Nollert assumed, without justification, an asymptotic approximation fo
r R-N(omega). This step is of some relevance since it opened to him the pos
sibility to compute, numerically, frequencies with a higher imaginary compo
nent than previous attempts. Here, we display a simple argument that justif
ies this procedure. We also show that our approach gives a dosed form for R
-N. The approximation displayed in this note for the computation of the qua
sinormal modes is straightforward. From our point of view, it reinforces th
e confidence on the clever numerical approaches introduced lately in this r
esearch area. [S0556-2821(99)01704-X].