Floquet Time Crystal — Period Doubling

Discrete time crystal in a periodically driven spin chain · Subharmonic response at 2T

Drive Parameters

Observables

Period T1
Response period
Magnetization ⟨σ⟩
Floquet cycle0
Phase

About

A Floquet time crystal breaks discrete time-translation symmetry: driven at period T, the system responds at 2T. This requires many-body localization (MBL) — disorder prevents thermalization. When g≈1 (π-pulse), spins flip each drive cycle and the magnetization oscillates at 2T. Above a threshold disorder the crystal phase persists; reduce disorder to melt it.