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The Thouless energy is a characteristic energy scale of diffusive disordered conductors. It is defined by $E_T=\hslash D/L^2$, where D is the diffusion constant and L the size of the system, and thereby inversely proportional to the diffusion time $t_D=L^2/D$ through the system.

It was first introduced by the Scottish-American physicist David J. Thouless when studying Anderson localization , as a measure of the sensitivity of energy levels to a change in the boundary conditions of the system. Though being a classical quantity, it has been shown to play an important role in the quantum-mechanical treatment of disordered systems.

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