Quench dynamics in three-level dipole-interacting Rydberg arrays produce scalable spin-nematic squeezing with ξ² ∝ N^{-2/3} (all-to-all symmetric) or N^{-0.7} (antisymmetric), yielding F_Q ∝ N².
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Resonant monopole-dipole energy transfer observed between Rydberg helium atoms and polar ammonia molecules at low temperature, quantitatively explained by charge-dipole interaction calculations.
The dynamical squeezing phase transition in bilayer XXZ spin models is universal across lattice geometries and interlayer coupling rescalings, with a new sub-linear scaling for short-range interactions.
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Observation of resonant monopole-dipole energy transfer between Rydberg atoms and polar molecules
Resonant monopole-dipole energy transfer observed between Rydberg helium atoms and polar ammonia molecules at low temperature, quantitatively explained by charge-dipole interaction calculations.