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@ARTICLE{Tasler:1048969,
author = {Tasler, Stephan and Old, Josias and Heunisch, Lukas and
Feulner, Verena and Eckstein, Timo and Müller, Markus and
Hartmann, Michael J.},
title = {{O}ptimizing {S}uperconducting {T}hree-{Q}ubit {G}ates for
{S}urface-{C}ode {E}rror {C}orrection},
reportid = {FZJ-2025-05066, arXiv:2506.09028},
year = {2025},
note = {12 pages, 11 figures},
abstract = {Quantum error correction (QEC) is one of the crucial
building blocks for developing quantum computers that have
significant potential for reaching a quantum advantage in
applications. Prominent candidates for QEC are stabilizer
codes for which periodic readout of stabilizer operators is
typically implemented via successive two-qubit entangling
gates, and is repeated many times during a computation. To
improve QEC performance, it is thus beneficial to make the
stabilizer readout faster and less prone to
fault-tolerance-breaking errors. Here we design a 3-qubit
CZZ gate for superconducting transmon qubits that maps the
parity of two data qubits onto one measurement qubit in a
single step. We find that the gate can be executed in a
duration of $35\,$ns with a fidelity of F$=99.96 \, \\%$. To
optimize the gate, we use an error model obtained from the
microscopic gate simulation to systematically suppress Pauli
errors that are particularly harmful to the QEC protocol.
Using this error model, we investigate the implementation of
this 3-qubit gate in a surface code syndrome readout
schedule. We find that for the rotated surface code, the
implementation of CZZ gates increases the error threshold by
nearly 50\\% to $\approx 1.2\,\\%$ and decreases the logical
error rate, in the experimental relevant regime, by up to
one order of magnitude, compared to the standard CZ readout
protocol. We also show that for the unrotated surface code,
strictly fault-tolerant readout schedules can be found. This
opens a new perspective for below-threshold surface-code
error correction, where it can be advantageous to use
multi-qubit gates instead of two-qubit gates to obtain a
better QEC performance.},
cin = {PGI-2},
cid = {I:(DE-Juel1)PGI-2-20110106},
pnm = {5221 - Advanced Solid-State Qubits and Qubit Systems
(POF4-522) / BMBF 13N16073 - MUNIQC-Atoms -
Neutralatom-basierter Quantencomputer-Demonstrator
(BMBF-13N16073)},
pid = {G:(DE-HGF)POF4-5221 / G:(DE-Juel1)BMBF-13N16073},
typ = {PUB:(DE-HGF)25},
eprint = {2506.09028},
howpublished = {arXiv:2506.09028},
archivePrefix = {arXiv},
SLACcitation = {$\%\%CITATION$ = $arXiv:2506.09028;\%\%$},
doi = {10.34734/FZJ-2025-05066},
url = {https://juser.fz-juelich.de/record/1048969},
}