Starting from recent observations about quasi-normal modes, we use semi-classical arguments to derive the Bekenstein-Hawking entropy spectrum ford-dimensional spherically symmetric black holes. We find that, as first suggested by Bekenstein, the entropy spectrum is equally spaced:
SBH = ln(m0) n
where m0 is a fixed integer that must be derived from the microscopic theory. For d-dimensional black holes of radius RH(M), our analysis predicts the form of the unique quasinormal mode frequency in the large damping limit. This prediction has been confirmed by recent calculations. These developments indicate that the classical quasi-normal modes are providing crucial information about the quantum gravitational states responsible for black hole entropy.