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Disorder in condensed matter can be represented by a random or a quasi-periodic potential, the second choice appearing naturally in cold atoms experiments. We consider a system of fermions on a lattice in d-dimensions with a many body interaction and a quasi-periodic disorder.
We prove that localization at strong disorder persists in the ground state in presence of a many body interaction. The proof relies on a combination of Renormalization Group methods with number theoretical properties (Diophantine conditions) similar to the ones assumed in KAM theory.
Link per il collegamento: https://meet.google.com/pip-kvzt-fkz
Giovanni Gallavotti