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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Scalable spin-nematic squeezing in multi-level dipole-interacting Rydberg atom arrays
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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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.
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Universal Spin Squeezing Dynamical Phase Transitions across Lattice Geometries, Dimensions, and Microscopic Couplings
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.