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This study demonstrates the feasibility of simulating complex many-body localization dynamics in Fermi-Hubbard systems using current noisy superconducting qubits, achieving significant circuit depth reductions through advanced compilation techniques like tensor-network optimization. By successfully mapping a 12-qubit correlated fermionic system to an IBM quantum processor and benchmarking results against exact simulations, the work highlights practical progress toward utilizing near-term hardware for fundamental condensed matter physics problems that are intractable on classical computers.
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Quantum computer-based simulation of Stark many-body localization in a 1D Fermi-Hubbard model

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arXiv:2608.02245v1 Announce Type: new Abstract: Many-body localization (MBL) is a dynamical phenomenon that describes the non-ergodicity of isolated quantum many-body systems. In contrast to thermalization, this phenomenon leads to a long-lived memory of initial states of local systems and slow growth of entanglement. In this work, we study Stark MBL in a 12-qubit correlated fermionic system described by the one-dimensional Fermi-Hubbard model using Hamiltonian simulation on an IBM superconducting qubit quantum computer. To enable such a computation on current-day noisy hardware, we combine a series of compilation steps, including the use of the spin-resolved Jordan-Wigner transformation, employing SWAP networks, and integrating a tensor-network-based quantum circuit optimization routine on top of a standard circuit optimization pipeline. As a result, there is approximately an 88$\%$ and 87$\%$ reduction in two-qubit gate count and circuit depth, respectively. Through such simulations of the real-time dynamics using Trotterized quantum circuits, we exhibit a crossover from thermalizing dynamics of the system at a weak tilt of the field to a strongly localized behavior at large tilt with short evolution times. We also benchmark our obtained results with respect to those from exact simulations.

Abstract:Many-body localization (MBL) is a dynamical phenomenon that describes the non-ergodicity of isolated quantum many-body systems. In contrast to thermalization, this phenomenon leads to a long-lived memory of initial states of local systems and slow growth of entanglement. In this work, we study Stark MBL in a 12-qubit correlated fermionic system described by the one-dimensional Fermi-Hubbard model using Hamiltonian simulation on an IBM superconducting qubit quantum computer. To enable such a computation on current-day noisy hardware, we combine a series of compilation steps, including the use of the spin-resolved Jordan-Wigner transformation, employing SWAP networks, and integrating a tensor-network-based quantum circuit optimization routine on top of a standard circuit optimization pipeline. As a result, there is approximately an 88$\%$ and 87$\%$ reduction in two-qubit gate count and circuit depth, respectively. Through such simulations of the real-time dynamics using Trotterized quantum circuits, we exhibit a crossover from thermalizing dynamics of the system at a weak tilt of the field to a strongly localized behavior at large tilt with short evolution times. We also benchmark our obtained results with respect to those from exact simulations.

Quantum Physics (quant-ph); Other Condensed Matter (cond-mat.other)

arXiv:2608.02245 [quant-ph]

(or arXiv:2608.02245v1 [quant-ph] for this version)

https://doi.org/10.48550/arXiv.2608.02245 Focus to learn more arXiv-issued DOI via DataCite (pending registration)

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