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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A coupled-channel framework based on Bogoliubov modes efficiently describes spinor BEC dynamics near spin-spatial resonances, classifying resonant excitations and showing that beyond-quadratic terms are needed for long-time behavior.
Exact dark-bright solitons exist in the integrable limit without spin-orbit coupling; finite couplings break integrability and produce spatial separation, density oscillations, and robust breathers in binary BECs.
Floquet driving of quadratic Zeeman energy in spin-2 BECs renormalizes angular-momentum-conserving spin-flip couplings via Bessel functions and produces enriched phase diagrams in driving-parameter space.
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Phase diagrams of spin-2 Floquet spinor Bose-Einstein condensates
Floquet driving of quadratic Zeeman energy in spin-2 BECs renormalizes angular-momentum-conserving spin-flip couplings via Bessel functions and produces enriched phase diagrams in driving-parameter space.