Related papers: Observing Two-Particle Correlation Dynamics in Tunable Superconducting Bose-Hubbard Simulators

Observing Two-Particle Correlation Dynamics in Tunable Superconducting Bose-Hubbard Simulators

URL: http://arxiv.org/abs/2509.02180v1
Date: Tue, 02 Sep 2025 10:44:59 GMT
Title: Observing Two-Particle Correlation Dynamics in Tunable Superconducting Bose-Hubbard Simulators
Authors: Z. T. Wang, Si-Yun Zhou, Yun-Hao Shi, Kaixuan Huang, Z. H. Yang, Jingning Zhang, Kui Zhao, Yueshan Xu, Hao Li, S. K. Zhao, Yulong Feng, Guangming Xue, Yu Liu, Wei-Guo Ma, Cai-Ping Fang, Hao-Tian Liu, Yong-Yi Wang, Kai Xu, Haifeng Yu, Heng Fan, S. P. Zhao,
Abstract summary: We experimentally study the two-particle correlation dynamics via quantum walks in superconducting Bose-Hubbard qutrit arrays.<n>Our work highlights the role of interaction in shaping quantum dynamics and extends the realm of simulating correlated quantum systems with superconducting circuits.
Score: 30.183205236173617
License: http://arxiv.org/licenses/nonexclusive-distrib/1.0/
Abstract: The generation and propagation of quantum correlations are central to understanding many dynamical properties of quantum systems, yet their precise experimental control and characterization remain a key challenge. Here we experimentally study the two-particle correlation dynamics via quantum walks in superconducting Bose-Hubbard qutrit arrays, with tunable on-site interaction $U$ realized by Floquet engineering. Quantum walks show the characteristic change from bosonic bunching to fermionic antibunching with increasing $U$. The two-particle entanglement and quantum correlation dynamics, as measured by negativity and quantum discord, are investigated. We find that depending on the initial state, the propagation of entanglement can be strongly suppressed with increasing $U$, while that of quantum discord exhibits considerably larger amplitude; or both of them appear insensitive to $U$. Furthermore, the forms of entanglement are found to persist throughout particle walks for $U =$ 0 and it is generally not the case when $U$ increases. Our work highlights the role of interaction in shaping quantum dynamics and extends the realm of simulating correlated quantum systems with superconducting circuits.

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