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Concretely: for๐‘”0 >0, the region sat- isfying๐œ† >โˆ’๐‘” 0 and๐œ† <โˆ’1/4belongs to the OSL; for ๐‘”0 <0the analogous region is๐œ† <โˆ’๐‘” 0 and๐œ† >+1/4

There exists a gapless spin-liquid region with very low fidelity at๐‘˜ 0 that we denote as the Oscillatory spinliquid 1 (OSL)

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Integrable Floquet Time Crystals in One Dimension

cond-mat.str-el ยท 2025-10-05 ยท unverdicted ยท novelty 5.0

Integrable Floquet time crystals realized in 1D quadratic lattice models from spin chains, with rigid DTC phase, phase diagram showing transitions to Floquet paramagnet, and exponentially diverging lifetime via finite-size scaling.

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  • Integrable Floquet Time Crystals in One Dimension cond-mat.str-el ยท 2025-10-05 ยท unverdicted ยท none ยท ref 7

    Integrable Floquet time crystals realized in 1D quadratic lattice models from spin chains, with rigid DTC phase, phase diagram showing transitions to Floquet paramagnet, and exponentially diverging lifetime via finite-size scaling.