Abstract:
We argue that semiconducting quenched liquids and frozen glasses may
exhibit a set of peculiar electronic states of topological
origin. These states reside at transient strained regions arising
during structural reconfigurations between distinct aperiodic states
intrinsic to quenched melts. The states are predominantly filled and
serve as a non-paramagnetic source of charge carriers that may alone
account for the observed magnitude of DC-conductivity.