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This research proposes a method to stabilize polar molecular mixtures using double microwave shielding, enabling tunable long-range dipolar interactions essential for quantum simulation. By suppressing collisional losses while maintaining state-dependent control over spin textures and Hubbard models, the work advances practical pathways toward realizing complex many-body physics in bulk gases and optical lattices.
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Tunable state-dependent interactions in collisionally stable mixtures of polar molecules

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arXiv:2607.25777v1 Announce Type: cross Abstract: We propose encoding a pseudo-spin-$1/2$ system in the ground ($v=0$) and first excited ($v=1$) vibrational states of polar molecules. Double microwave shielding simultaneously shields molecules in both states, suppressing two-body losses by orders of magnitude while strictly avoiding three-body recombination. The microwave dressing is state-dependent and results in highly tunable, long-range dipolar Ising exchange ($J_z$), density-density ($V$), and spin-density ($W$) interactions. These interaction length scales readily exceed the typical interparticle spacing, pushing the molecules deep into the strongly interacting regime. In bulk gases, this enables the exploration of itinerant quantum magnetism and quantum droplets with novel anisotropic spin textures; in optical lattices, it naturally realizes extended Hubbard and $t$-$J_z$ models, opening new directions in quantum simulation.

Abstract:We propose encoding a pseudo-spin-$1/2$ system in the ground ($v=0$) and first excited ($v=1$) vibrational states of polar molecules. Double microwave shielding simultaneously shields molecules in both states, suppressing two-body losses by orders of magnitude while strictly avoiding three-body recombination. The microwave dressing is state-dependent and results in highly tunable, long-range dipolar Ising exchange ($J_z$), density-density ($V$), and spin-density ($W$) interactions. These interaction length scales readily exceed the typical interparticle spacing, pushing the molecules deep into the strongly interacting regime. In bulk gases, this enables the exploration of itinerant quantum magnetism and quantum droplets with novel anisotropic spin textures; in optical lattices, it naturally realizes extended Hubbard and $t$-$J_z$ models, opening new directions in quantum simulation.

Quantum Gases (cond-mat.quant-gas); Atomic Physics (physics.atom-ph); Chemical Physics (physics.chem-ph); Quantum Physics (quant-ph)

arXiv:2607.25777 [cond-mat.quant-gas]

(or arXiv:2607.25777v1 [cond-mat.quant-gas] for this version)

https://doi.org/10.48550/arXiv.2607.25777 Focus to learn more arXiv-issued DOI via DataCite (pending registration)

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