
Time quasicrystals provide a controllable, long‑lived non‑equilibrium state, opening pathways for resilient quantum sensors and information processors while expanding the landscape of observable phases in driven‑dissipative systems.
Time crystals, first proposed as periodically ordered states that break temporal symmetry, have reshaped our understanding of non‑equilibrium physics. Extending this concept, time quasicrystals exhibit order without strict periodicity, mirroring the spatial aperiodicity of classic quasicrystals. Achieving such phases requires a delicate balance between external driving and internal dissipation, a regime that has remained largely theoretical until recent experimental advances. By employing a quasi‑periodic Fibonacci sequence as the drive, researchers can imprint a complex temporal pattern while still allowing the system to settle into a stable, ordered rhythm. In the new work, Anisur and Choudhury applied a Fibonacci drive to the open Dicke model—a collection of qubits coupled to a lossy cavity—and observed a clear sub‑harmonic response that does not mirror the input sequence. Crucially, the time‑quasicrystal signature survived even when only two qubits were present, defying the expectation that many‑body interactions are required. Systematic simulations revealed that the lifetime τ* scales linearly with the number of qubits, indicating that larger ensembles can host increasingly robust temporal order. These results were validated through decorrelator and quasicrystal‑fraction metrics, establishing a firm thermodynamic‑limit picture. The ability to generate long‑lived, dissipative time‑quasicrystals opens several avenues for quantum technology. Stable non‑equilibrium states could serve as reference clocks for quantum sensing, improve error‑resilient gates, or enable novel information‑storage schemes that exploit temporal patterns rather than spatial configurations. Moreover, the demonstrated scalability suggests that similar protocols might be adapted to other platforms such as trapped ions or superconducting circuits. Ongoing challenges include capturing deep quantum effects beyond mean‑field approximations and engineering precise quasi‑periodic drives in noisy environments, but the present findings lay a solid foundation for exploring these frontiers.
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