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Since the energy ofP 4 is always lower thanP 0 andP 2,P 4 becomes ground state in the region of−˜c 2/2< q 0 <˜c2/2

For the polar stateP 4,γ= p (2q0 + ˜c0)/2˜c2 andp (1−γ 2)/2 = p (˜c2 −2q 0)/4˜c2, the existence of which requires−˜c2/2< q 0 <˜c2/2

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Phase diagrams of spin-2 Floquet spinor Bose-Einstein condensates

cond-mat.quant-gas · 2025-10-19 · unverdicted · novelty 5.0

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 cond-mat.quant-gas · 2025-10-19 · unverdicted · none · ref 3

    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.