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Consequently, only ๐œ”๐‘Ž๐‘ก ๐ฝ๐‘ฅ/๐œ”๐‘Ž 0 10 โˆ’1 1 0 0.12 ๐ธ/๐œ”๐‘Ž 0 0.016๐ธ/๐œ”๐‘Ž 0.09 0 ๐ธ/๐œ”๐‘Ž ๐œ”๐‘Ž๐‘ก ๐ฝ๐‘ฆ/๐œ”๐‘Ž 0 10 โˆ’1 1 ๐œ”๐‘Ž๐‘ก ๐ฝ๐‘ง/๐œ”๐‘Ž 0 10 โˆ’1 1 (a) (b) (c) (d) (e) (f) Figure 2

generates no spin squeezing in either regime, purely modifies the effective detuning โˆ† z

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Spin-Squeezing-Enhanced Charging for Quantum Dicke Batteries

quant-ph ยท 2026-06-30 ยท unverdicted ยท novelty 6.0

Transverse interactions in Dicke QBs induce collective spin squeezing for exponential coupling boost and act as nonlinear torque to guide optimal charging paths, remaining robust under dissipation and sometimes outperforming ideal cases.

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  • Spin-Squeezing-Enhanced Charging for Quantum Dicke Batteries quant-ph ยท 2026-06-30 ยท unverdicted ยท none ยท ref 1

    Transverse interactions in Dicke QBs induce collective spin squeezing for exponential coupling boost and act as nonlinear torque to guide optimal charging paths, remaining robust under dissipation and sometimes outperforming ideal cases.