Results are presented from theoretical investigations of condensed excited states of beryllium by the Hartree-Fock method with allowance for the width of the atomic levels. It is shown that, during the excitation of a beryllium atom in the X-ray energy range, the 2p states split, the one-electron energy levels are shifted by unequal amounts, the 2s and 2p states mix at excitation energies of 10 and 14 Ry, and the atom is stabilized at energies higher than 6.7 Ry. In the optical range of excitation energies, a condensed excited state of beryllium with a lifetime on the order of 0.1 fs is revealed.