Abstract
The transition rates of individual two-state systems in a mesoscopic disordered metal (Bi) are studied via time-dependent conductance fluctuations. A striking increase in the transition rates is observed as the temperature T is decreased below 1 K for defects with energy splitting ɛ<kBT. In contrast, the transition rates decrease monotonically as T is lowered if ɛ>kBT. We show that these phenomena are a manifestation of dissipative quantum tunneling and estimate, for one particular defect, the defect–conduction-electron coupling parameter, α≊0.24.

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