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This research presents a scalable algorithm using tensor networks and influence martingales to simulate non-Markovian dynamics in large quantum spin chains, effectively addressing the exponential complexity of open quantum systems. By introducing an "influence radius" concept, the method enables efficient modeling of memory effects in systems up to 100 qubits, advancing classical simulation capabilities for quantum physics.
Tensor-Network-Based Unraveling of Non-Markovian Dynamics in Large Spin Chains via the Influence Martingale Approach
arXiv:2510.11200v4 Announce Type: replace Abstract: Classical simulation of open quantum system dynamics remains challenging due to the exponential growth of the Hilbert space, the need to accurately capture dissipation and decoherence, and the added complexity of memory effects in the non-Markovian regime. We develop an efficient algorithm for simulating both Markovian and non-Markovian dynamics in large one-dimensional quantum systems. Extending the Tensor Jump Method, which combines TDVP-based tensor-network evolution with a Suzuki--Trotter decomposition of stochastic trajectories, our approach incorporates time-dependent decay rates--treating positive rates as time-inhomogeneous Markovian processes and negative rates via the Influence Martingale formalism to unravel time-local non-Markovian dynamics. We further introduce the concept of the `influence radius' to achieve a resource-efficient framework enabling scalable simulations of open-system dynamics in the non-Markovian regime, as demonstrated for a one-dimensional transverse-field Ising chain comprising up to 100 spin qubits.
Abstract:Classical simulation of open quantum system dynamics remains challenging due to the exponential growth of the Hilbert space, the need to accurately capture dissipation and decoherence, and the added complexity of memory effects in the non-Markovian regime. We develop an efficient algorithm for simulating both Markovian and non-Markovian dynamics in large one-dimensional quantum systems. Extending the Tensor Jump Method, which combines TDVP-based tensor-network evolution with a Suzuki--Trotter decomposition of stochastic trajectories, our approach incorporates time-dependent decay rates--treating positive rates as time-inhomogeneous Markovian processes and negative rates via the Influence Martingale formalism to unravel time-local non-Markovian dynamics. We further introduce the concept of the `influence radius' to achieve a resource-efficient framework enabling scalable simulations of open-system dynamics in the non-Markovian regime, as demonstrated for a one-dimensional transverse-field Ising chain comprising up to 100 spin qubits.
arXiv:2510.11200 [quant-ph]
(or arXiv:2510.11200v4 [quant-ph] for this version)
https://doi.org/10.48550/arXiv.2510.11200 Focus to learn more arXiv-issued DOI via DataCite
Phys. Rev. A 114, 032445 (21 September, 2026)
https://doi.org/10.1103/8y3g-jdjx Focus to learn more DOI(s) linking to related resources
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