Lieb's Theorem and Maximum Entropy Condensates
Year: 2021
Type: article
Abstract: Coherent driving has established itself as a powerful tool for guiding a many-body quantum system into a desirable, coherent non-equilibrium state. A thermodynamically large system will, however, almost always saturate to a featureless infinite temperature state under continuous driving and so the optical manipulation of many-body systems is considered feasible only if a transient, prethermal regime exists, where heating is suppressed. Here we show that, counterintuitively, in a broad class of lattices Floquet heating can actually be an advantageous effect. Specifically, we prove that the maximum entropy steady states which form upon driving the ground state of the Hubbard model on unbalanced bi-partite lattices possess uniform off-diagonal long-range order which remains finite even in the thermodynamic limit. This creation of a `hot' condensate can occur on any driven unbalanced lattice and provides an understanding of how heating can, at the macroscopic level, expose and alter the order in a quantum system. We discuss implications for recent experiments observing emergent superconductivity in photoexcited materials.
Source: Quantum
Language: English
Topic: Quantum many-body systems
Subfield: Atomic and Molecular Physics, and Optics
Field: Physics and Astronomy
Domain: Physical Sciences
Open Access status: gold
Estimated APC paid: $215
Awards: G1045617361, G1230266125, G3207356259, EXC 2056: CUI: Advanced Imaging of Matter, G393177772, Designing Out-of-Equilibrium Many-Body Quantum Systems, G4675369358, G4760961572, G5586663373, G5631081224, G5692702728, G5702163051, Tensor Network Theory for strongly correlated quantum systems, G6184482982, G8205271416
OpenAlex ID: W3135021460
