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Discrete time crystals are periodically driven systems characterized by a response with periodicity $nT$, with $T$ the period of the drive and $n>1$.
Shunted-josephson-junction model. ii. the nonautonomous case
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Phase locking, period doubling bifurcations and chaos in a mathematical model of a periodically driven oscillator: A theory for the entrainment of biological oscillators and the generation of cardiac dysrhythmias
Guevara, M. R. & Glass, L · 1982
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Complete devil’s staircase, fractal dimension, and universality of mode-locking structure in the circle map
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Cosme, J. G. & Fialko, O · 2014
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Floquet time crystals
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Phase structure of one-dimensional interacting floquet systems. ii. symmetry-broken phases
von Keyserlingk, C. W. & Sondhi, S. L · 2016
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Absolute stability and spatiotemporal long-range order in floquet systems
von Keyserlingk, C. W., Khemani, V. & Sondhi, S. L · 2016
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Phase structure of driven quantum systems
Khemani, V., Lazarides, A., Moessner, R. & Sondhi, S. L · 2016
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Parafermion chain with 2 π \pi /k floquet edge modes
Sreejith, G. J., Lazarides, A. & Moessner, R · 2016
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Time crystals: a review
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Floquet time crystal in the lipkin-meshkov-glick model
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Prethermal phases of matter protected by time-translation symmetry
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Discrete time crystals: rigidity, criticality, and realizations
Yao, N. Y., Potter, A. C., Potirniche, I.-D. & Vishwanath, A · 2017
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Dynamical quantum phase transitions: A brief survey
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Else, D. V., Monroe, C., Nayak, C. & Yao, N. Y · 2019
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Dicke time crystals in driven-dissipative quantum many-body systems
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Observation of a discrete time crystal
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Floquet time crystals in clock models
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Long-lived interacting phases of matter protected by multiple time-translation symmetries in quasiperiodically driven systems
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