Hilbert Space Fragmentation from Generalized Symmetries
Thea Budde, Marina Kristć Marinković, Joao C. Pinto Barros
TLDR
Generalized symmetries can cause Hilbert space fragmentation, demonstrating that it doesn't always imply ergodicity breaking.
Key contributions
- Generalized symmetries (higher-form, subsystem, gauge) cause exponential Hilbert space fragmentation.
- Non-invertible symmetries induce additional fragmentation within individual symmetry sectors.
- Exponentially many Krylov sectors alone do not imply ergodicity breaking.
- Disorder-free localization can arise from Krylov-restricted thermalization without ergodicity breaking.
Why it matters
This paper fundamentally redefines our understanding of Hilbert space fragmentation, showing that generalized symmetries can cause it. It challenges the long-held assumption that exponential fragmentation always implies ergodicity breaking, impacting the classification of quantum many-body systems.
Original Abstract
Hilbert space fragmentation refers to exponential growth in the number of dynamically disconnected Krylov sectors with system size. It is taken as evidence of ergodicity breaking, since conventional symmetries generate at most a polynomial number of sectors. However, we demonstrate that generalized symmetries can fragment the Hilbert space. Models with higher-form, subsystem, and gauge symmetries can have exponentially many symmetry sectors. We further prove that non-invertible symmetries can induce additional fragmentation within individual symmetry sectors. Fragmentation in several known models arises from generalized symmetries, and the presence of exponentially many Krylov sectors therefore does not by itself imply ergodicity breaking. Finally, we show that disorder free localization arises naturally from Krylov-restricted thermalization when sectors lack translation invariance, requiring neither ergodicity breaking nor gauge symmetry.
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