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This study establishes the relationship between Krylov complexity and Berry phase in adiabatic dynamics, showing how non-vanishing complexity arises from superposition states rather than instantaneous eigenstates. The research reveals that for single qubit systems with constant parameters, this complexity oscillates harmonically at a frequency determined by external field strength and geometric phases. These findings advance the theoretical understanding of quantum information scrambling in slowly evolving spin systems without relying on AI or machine learning methods.
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Krylov complexity and Berry phase in quantum adiabatic dynamics

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arXiv:2608.14325v1 Announce Type: new Abstract: The connection between Krylov complexity and Berry phase in adiabatic dynamics is investigated under the instantaneous eigenstate basis of a slowly evolving spin system. Adiabatic dynamics force the Krylov complexity to vanish if the initial Krylov basis is an instantaneous eigenstate of the Hamiltonian. Nevertheless, we demonstrate that the Krylov complexity will be nonvanishing if the initial Krylov basis is a superposition state rather than an eigenstate. Time evolution of Krylov complexity will behave periodically or quasi-periodically depending on the controlling parameters. In particular, for a single qubit system with constant parameters, the Krylov complexity will oscillate harmonically in time with the frequency relevant to the combination of the strength of the external field and the geometric Berry phase.

Abstract:The connection between Krylov complexity and Berry phase in adiabatic dynamics is investigated under the instantaneous eigenstate basis of a slowly evolving spin system. Adiabatic dynamics force the Krylov complexity to vanish if the initial Krylov basis is an instantaneous eigenstate of the Hamiltonian. Nevertheless, we demonstrate that the Krylov complexity will be nonvanishing if the initial Krylov basis is a superposition state rather than an eigenstate. Time evolution of Krylov complexity will behave periodically or quasi-periodically depending on the controlling parameters. In particular, for a single qubit system with constant parameters, the Krylov complexity will oscillate harmonically in time with the frequency relevant to the combination of the strength of the external field and the geometric Berry phase.

Quantum Physics (quant-ph); Other Condensed Matter (cond-mat.other); High Energy Physics - Theory (hep-th)

arXiv:2608.14325 [quant-ph]

(or arXiv:2608.14325v1 [quant-ph] for this version)

https://doi.org/10.48550/arXiv.2608.14325 Focus to learn more arXiv-issued DOI via DataCite (pending registration)

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