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Flux Magnetism in a Strongly Interacting Dipolar Lattice Supersolid under Tunable Gauge Fields
Phys. Rev. Lett. 137, 043401 – Published 22 July, 2026
DOI: https://doi.org/10.1103/tbp3-7rh3
Abstract
Supersolidity and magnetism are fundamental phenomena characterizing strongly correlated matter. Here we unveil a mechanism that directly connects these two regimes and can be experimentally accessed in ultracold atomic systems. Specifically, we exploit the distinctive properties of magnetic lanthanide atoms trapped in a one-dimensional antimagic wavelength optical lattice. This platform enables a realistic implementation of a triangular Bose-Hubbard ladder featuring two key ingredients: strong long-range interactions and tunable gauge fields. Owing to these properties, our numerical analysis reveals a robust lattice supersolid regime with finite fluxes in each triangular plaquette. Remarkably, we show that the density modulation of the supersolid phase and a finite gauge field induce magnetic ordering of the fluxes, forming ferromagnetic and ferrimagnetic patterns. Our results thus reveal a quantum effect that bridges supersolidity and magnetism.
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For a triangular ladder with sites, the sum of and plaquettes is . Furthermore, the ground state of the lattice SS phase is twofold degenerate, reflecting the equal probability of having high occupations in even or odd sites. Since we chose to be odd in order to lift this degeneracy, we exclude a plaquette in the calculation: this allows us to consider the same number of and plaquettes, thus justifying the factor in Eq. (7).
Here we find only , consistent with a homogeneous superfluid.
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In the text we selected the configuration favoring high occupation in odd sites, while the opposite one would imply and therefore .
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