Temperature and frequency dependencies of DC and AC conductivities, dielectric response, static permittivity, optical absorption edge, infrared absorption spectrum, density, and temperatures of glass transition and crystallization for lithium molybdenum-antimonite glasses, (80 − x)Sb 2 O 3 -20Li 2 O-xMoO 3 , where x = 0-40, are measured and discussed. The DC conductivity increases with increasing concentration of MoO 3 . At 150°C, it ranges from 5 × 10 −11 S/m up to 3 × 10 −8 S/m. Polaron hopping between Mo 5+ and Mo 6+ ions contributes, probably, to the DC conductivity. Ionic conductivity by Li + ions is also present. The conduction activation energy monotonously decreases from 1.15 eV, at x = 5, down to 0.91 eV, at x = 40. In all glasses with x N 0, the conduction activation energy is close to a half of the indirect allowed optical gap. The pre-exponential factor, σ 0 , goes through a sharp maximum close to the composition (x = 20) with both the highest glass transition temperature and the largest thermal stability range. The frequency dependence of the AC conductivity is composed of three components -the DC conductivity and two AC components. For x = 35 and 40, the activation energy of electrical relaxation is equal to 0.954 ± 0.008 eV and the pre-exponential factor of relaxation times is equal to (4 ± 1) 10 −14 s. The static relative permittivity ranges from 17.4 to 23.0. Strong extrinsic absorption bands in infrared region originate from hydroxyl ions, CO 2 impurities, and silicon-oxygen vibrations. The UV-visible indirect allowed absorption edge shifts from 2.6 eV to 2.1 eV with increasing MoO 3 content. With increasing MoO 3 content the glasses darken, from a light yellow color, at x = 0, to a deep brown color, at x = 40.