ﻻ يوجد ملخص باللغة العربية
Coherent driving has established itself as a powerful tool for guiding a many-body quantum system into a desirable, correlated pre-thermal regime. The focus on this transient regime where heating is slow is a result of the intuition that a thermodynamically large system will inevitably saturate to a featureless infinite temperature state under continuous driving. Here we show that whether or not Floquet heating is a deleterious effect actually depends on the geometry of the system. 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 expose order which has been suppressed by the lattice geometry. We discuss implications for recent experiments observing emergent superconductivity in photoexcited materials.
The noninteracting electronic structures of tight binding models on bipartite lattices with unequal numbers of sites in the two sublattices have a number of unique features, including the presence of spatially localized eigenstates and flat bands. Wh
One of the biggest puzzles concerning the cuprate high temperature superconductors is what determines the maximum transition temperature (Tc,max), which varies from less than 30 K to above 130 K in different compounds. Despite this dramatic variation
We show that Liebs concavity theorem holds more generally for any unitarily invariant matrix function $phi:mathbf{H}^n_+rightarrow mathbb{R}$ that is monotone and concave. Concretely, we prove the joint concavity of the function $(A,B) mapstophibig[(
The heavy-electron superconductor CeCoIn$_5$ exhibits a puzzling precursor state above its superconducting critical temperature at $T_c$ = 2.3 K. The thermopower and Nernst signal are anomalous. Below 15 K, the entropy current of the electrons underg
Mappings between models may be obtained by unitary transformations with preservation of the spectra but in general a change in the states. Non- canonical transformations in general also change the statistics of the operators involved. In these cases