- Open Access
Critically Slow Hilbert-Space Ergodicity in Quantum Morphic Drives
Phys. Rev. Lett. 135, 140402 – Published 29 September, 2025
DOI: https://doi.org/10.1103/dmfd-lgcq
Abstract
The maximum entropy principle is foundational for statistical analyses of complex dynamics. This principle has been challenged by the findings of a previous work [Phys. Rev. X 7, 031034 (2017)], where it was argued that a quantum system driven in time by a certain aperiodic sequence without any explicit symmetries, dubbed the Thue-Morse drive, gives rise to emergent nonergodic steady states which are underpinned by effective conserved quantities. Here, we resolve this apparent tension. We rigorously prove that the Thue-Morse drive achieves a very strong notion of quantum ergodicity in the long-time limit: The time evolution of any initial state uniformly visits every corner of its Hilbert space. On the other hand, we find the dynamics also approximates a Floquet drive for arbitrarily long, albeit finite periods of time with no characteristic timescale, resulting in a scale-free ergodic dynamics we call critically slow complete Hilbert-space ergodicity. Furthermore, numerical studies reveal that critically slow complete Hilbert-space ergodicity is not specific to the Thue-Morse drive and is, in fact, exhibited by many other aperiodic drives derived from morphic sequences, i.e., words derived from repeatedly applying substitution rules on basic characters. Our Letter presents a new class of dynamics in time-dependent quantum systems where full ergodicity is eventually attained but only after astronomically long times.
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We note that in previous physics literature it has been mischaracterized as such.
An analogous definition can apply for dynamics over continuous time as well.
The trace norm is defined as , where are the singular values of .
The trace distance is used because it gives the probability of distinguishing from a Haar-random state using an optimal, possibly entangling measurement over copies, so the requirement for all means that the late-time state is indistinguishable from Haar-random, even with access to an arbitrarily large number of system replicas and entangling measurements.
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With respect to the uniform measure on the semi-infinite cylinder.
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This is unlike the TMW, which is cube-free [33]—no word appears repeated more that twice.