Barely insulating disordered solids have the electronic states localiz
ed. Analyzing the density of states (DOS) by taking into account Coulo
mb correlations results in a particularity both on the metallic and on
the insulating side of the disorder-driven metal-insulator transition
(MIT): Coulomb interactions deplete the DOS near the Fermi energy E-F
. Efros and Shklovskii [1] pointed out that for solids on the insulati
ng side of the MIT at T = 0. long-range Coulomb interactions lead to t
he formation of a Coulomb gap. The DOS decreases then with a power law
when the energy approaches EF. TO investigate the density of states a
t E-F of n-type germanium we tried tunneling spectroscopy using mechan
ically-controllable break junctions [2] down to 100 mK. The tunneling
conductance was found to depend strongly on energy and temperature. We
analyze these experiments together with the bulk electrical resistivi
ty.