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Simulating Schwinger model dynamics with quasi-one-dimensional qubit arrays

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arxiv 2409.14544 v1 pith:NA6JVGNQ submitted 2024-09-22 quant-ph cond-mat.quant-gascond-mat.str-elhep-lathep-ph

classification quant-phcond-mat.quant-gascond-mat.str-elhep-lathep-ph
keywords modeldynamicsquantumschwingerprocessesarrayarraysepsilon
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abstract

Real-time dynamics of the Schwinger model provide an effective description of quark confinement out of equilibrium, routinely employed to model hadronization processes in particle-physics event generators. Ab-initio simulations of such non-perturbative processes are far beyond the reach of existing computational tools, and remain an outstanding open quest for quantum simulators to date. In this work we develop a general strategy to run Schwinger model dynamics on synthetic quantum spin lattices, such as neutral-atom or superconducting-qubit arrays. Our construction encodes the constrained fermionic and bosonic degrees of freedom of the model into the geometric shape of a magnetic interface. We show that global magnetic field patterns can drive coherent quantum dynamics of the interface equivalent to the lattice Schwinger Hamiltonian. We rigorously establish that the optimal array required for simulating real-time wave packet collisions and string fragmentation processes with accuracy $\epsilon$ in the continuum field-theory limit, is a quasi-one-dimensional ribbon with polynomial length and polylogarithmic width in $\epsilon^{-1}$. We finally discuss a concrete advantageous implementation using a state-of-the-art dual-species Rydberg atom array. This work opens up a path for near-term quantum simulators to address questions of immediate relevance to particle physics.

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  1. Interface phases and dynamics in two-dimensional quantum magnets: A "holographic" approach from universality to quantum simulation

    cond-mat.stat-mech 2026-08 conditional novelty 7.0 of 10

    Interface fluctuations in 2D quantum magnets are shown to encode the full phase diagram and transport universality classes of 1D spin chains, with a local-measurement protocol for reading out 1D full counting statistics.

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