Abstract

Normally the role of phase fluctuations in superfluids and superconductors is to drive a phase transition to the normal state. This happens due to proliferation of topologically nontrivial phase fluctuations in the form of vortices. Here we discuss a class of systems where, by contrast, nontopological phase fluctuations can produce superfluidity. Here we understand superfluidity as a phenomenon that does not necessarily arises from a broken U(1)U(1) symmetry, but can be associated with a certain class of (approximate or exact) degeneracies of the systems energy landscape giving raise to a U(1)U(1)-like phase.

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