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Flux Magnetism in a Strongly Interacting Dipolar Lattice Supersolid under Tunable Gauge Fields

Michele Miotto1,*, Pietro Lombardi2,3, Giovanni Ferioli4, Joana Fraxanet5, Maciej Lewenstein5,6, Luca Tanzi2,3, and Luca Barbiero7,†

  • *Contact author: m.miotto@tu-berlin.de
  • †Contact author: luca.barbiero@polito.it

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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