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Concurrent VQE for Simulating Excited States of the Schwinger Model

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arxiv 2407.15629 v1 pith:S47AYX5J submitted 2024-07-22 quant-ph cond-mat.str-elhep-lat

classification quant-phcond-mat.str-elhep-lat
keywords statesexcitedquantumqubitsancillarycircuitsconcurrentcvqe
verification ladder T0 review T1 audit T2 compute T3 formal
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abstract

This work explores the application of the concurrent variational quantum eigensolver (cVQE) for computing excited states of the Schwinger model. By designing suitable ansatz circuits utilizing universal SO(4) or SO(8) qubit gates, we demonstrate how to efficiently obtain the lowest two, four, and eight eigenstates with one, two, and three ancillary qubits for both vanishing and non-vanishing background electric field cases. Simulating the resulting quantum circuits classically with tensor network techniques, we demonstrate the capability of our approach to compute the two lowest eigenstates of systems with up to $\mathcal{O}(100)$ qubits. Given that our method allows for measuring the low-lying spectrum precisely, we also present a novel technique for estimating the additive mass renormalization of the lattice based on the energy gap. As a proof-of-principle calculation, we prepare the ground and first-excited states with one ancillary and four physical qubits on quantum hardware, demonstrating the practicality of using the cVQE to simulate excited states.

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Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Critical behavior of the Schwinger model via gauge-invariant VUMPS

    hep-lat 2024-12 conditional novelty 6.0 of 10

    The gauge-invariant VUMPS algorithm determines the continuum critical mass of the Schwinger model as (m/g)c = 0.333556(5) and produces data collapse consistent with Ising critical exponents.

  2. Meson thermalization with a hot medium in the open Schwinger model

    hep-lat 2025-01 conditional novelty 4.0 of 10

    Tensor-network simulations of the open Schwinger model show that meson thermalization time grows with dissipation strength, temperature, background electric field, and fermion mass.

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