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This research outlines a protocol for generating singlet Bell states using analogue superconducting devices governed by the transverse-field Ising model, leveraging direct Hamiltonian control rather than standard gate sequences. By utilizing adiabatic interpolation and resonant population transfer, the method achieves fidelities comparable to conventional approaches within approximately 100 nanoseconds while maintaining robustness against systematic errors. The study demonstrates that high-fidelity entanglement preparation is feasible in analogue architectures without requiring excessive duration or complex error correction overheads.
Preparation of a Bell state in an analogue device hosting the transverse-field Ising model
arXiv:2609.09013v1 Announce Type: new Abstract: We propose a protocol for preparing the singlet Bell state in an analogue device implementing the transverse-field Ising model with ZZ interactions and local X and Z fields, which can be engineered within the superconducting platform, among others. This protocol is performed by direct control of the terms of the Hamiltonian alone. The method exploits the fact that the singlet state is the first excited state of a symmetric Hamiltonian family, and comprises two steps: an adiabatic interpolation preparing the ground state of said symmetric Hamiltonian, followed by the resonant population transfer between its two lowest energy levels. For realistic parameters, the protocol achieves fidelities comparable to standard gate-based preparation within similar time scales ($\sim$100 ns), and can reach infidelities on the order of $10^{-4}$ with a moderately increased duration. We further analyse robustness against systematic control errors and show that high fidelities are maintained under implementation imperfections.
Abstract:We propose a protocol for preparing the singlet Bell state in an analogue device implementing the transverse-field Ising model with ZZ interactions and local X and Z fields, which can be engineered within the superconducting platform, among others. This protocol is performed by direct control of the terms of the Hamiltonian alone. The method exploits the fact that the singlet state is the first excited state of a symmetric Hamiltonian family, and comprises two steps: an adiabatic interpolation preparing the ground state of said symmetric Hamiltonian, followed by the resonant population transfer between its two lowest energy levels. For realistic parameters, the protocol achieves fidelities comparable to standard gate-based preparation within similar time scales ($\sim$100 ns), and can reach infidelities on the order of $10^{-4}$ with a moderately increased duration. We further analyse robustness against systematic control errors and show that high fidelities are maintained under implementation imperfections.
arXiv:2609.09013 [quant-ph]
(or arXiv:2609.09013v1 [quant-ph] for this version)
https://doi.org/10.48550/arXiv.2609.09013 Focus to learn more arXiv-issued DOI via DataCite (pending registration)
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Full text under the publisher's open licence · 239 words
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