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Localization transitions as a function of temperature require a many-body mobility edge in energy, separating localized from ergodic states.
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We believe that, in the thermodynamic limit, the presence of finite conduction implies ergodicity, too. This follows if one disregards the exotic scenario of non-ergodic, but delocalized many-body systems, where transport is confined to a fractal support in real space. Indeed, in large enough systems, delocalized modes supported on a finite fraction of space will serve as a bath, which is expected to thermalize any finite set of degrees of freedom in finite times
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