Superconducting architecture demonstrating fast, tunable high-fidelity <i>CZ</i> gates with parametric control of <i>ZZ</i> coupling

Future quantum information processors require tunable coupling architectures that can produce high-fidelity logical gates between two or more qubits. Parametric coupling is a powerful technique for generating tunable interactions between many qubits. Here, we present a highly flexible parametric coupling scheme with superconducting qubits that provides complete removal of residual <a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"> <a:mi>Z</a:mi> <a:mi>Z</a:mi> </a:math> coupling and the implementation of driven SWAP or SWAP-free controlled- <c:math xmlns:c="http://www.w3.org/1998/Math/MathML" display="inline"> <c:mi>Z</c:mi> </c:math> ( <e:math xmlns:e="http://www.w3.org/1998/Math/MathML" display="inline"> <e:mi>C</e:mi> <e:mi>Z</e:mi> </e:math> ) gates. Our fully integrated two-dimensional on-chip coupler design is only weakly flux tunable, cancels static linear coupling between the qubits, avoids internal coupler dynamics or excitations, and is extensible to multiqubit circuit-QED systems. Exploring gate fidelity versus gate duration allows us to maximize two-qubit gate fidelity, while providing insights into possible error sources for these gates. Randomized benchmarking over several hours reveals that the parametric SWAP <g:math xmlns:g="http://www.w3.org/1998/Math/MathML" display="inline"> <g:mi>C</g:mi> <g:mi>Z</g:mi> </g:math> gate achieves an average fidelity of <i:math xmlns:i="http://www.w3.org/1998/Math/MathML" display="inline"> <i:mn>99.44</i:mn> <i:mo>±</i:mo> <i:mn>0.09</i:mn> <i:mi mathvariant="normal">%</i:mi> </i:math> in a gate duration of 70 ns and that a dispersively driven parametric SWAP-free <l:math xmlns:l="http://www.w3.org/1998/Math/MathML" display="inline"> <l:mi>C</l:mi> <l:mi>Z</l:mi> </l:math> gate attains an average fidelity of <n:math xmlns:n="http://www.w3.org/1998/Math/MathML" display="inline"> <n:mn>99.47</n:mn> <n:mo>±</n:mo> <n:mn>0.07</n:mn> <n:mi mathvariant="normal">%</n:mi> </n:math> in only 30 ns. The fidelity remained above this value for over 8 h and peaked twice with a maximum of <q:math xmlns:q="http://www.w3.org/1998/Math/MathML" display="inline"> <q:mn>99.67</q:mn> <q:mo>±</q:mo> <q:mn>0.14</q:mn> <q:mi mathvariant="normal">%</q:mi> </q:math> . Overall, our parametric approach combines versatility, precision, speed, and high performance in one compact coupler design.

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Publication Details

Journal
Physical Review Applied
Published
2025-10-21
DOI
https://doi.org/10.1103/kmls-lgp5
Primary Topic
Quantum Computing Algorithms and Architecture
Type
article
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article

Superconducting architecture demonstrating fast, tunable high-fidelity CZ gates with parametric control of ZZ coupling

Physical Review Applied
Quantum Computing Algorithms and Architecture
article

Superconducting architecture demonstrating fast, tunable high-fidelity CZ gates with parametric control of ZZ coupling

article en

Abstract

Future quantum information processors require tunable coupling architectures that can produce high-fidelity logical gates between two or more qubits. Parametric coupling is a powerful technique for generating tunable interactions between many qubits. Here, we present a highly flexible parametric coupling scheme with superconducting qubits that provides complete removal of residual <a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"> <a:mi>Z</a:mi> <a:mi>Z</a:mi> </a:math> coupling and the implementation of driven SWAP or SWAP-free controlled- <c:math xmlns:c="http://www.w3.org/1998/Math/MathML" display="inline"> <c:mi>Z</c:mi> </c:math> ( <e:math xmlns:e="http://www.w3.org/1998/Math/MathML" display="inline"> <e:mi>C</e:mi> <e:mi>Z</e:mi> </e:math> ) gates. Our fully integrated two-dimensional on-chip coupler design is only weakly flux tunable, cancels static linear coupling between the qubits, avoids internal coupler dynamics or excitations, and is extensible to multiqubit circuit-QED systems. Exploring gate fidelity versus gate duration allows us to maximize two-qubit gate fidelity, while providing insights into possible error sources for these gates. Randomized benchmarking over several hours reveals that the parametric SWAP <g:math xmlns:g="http://www.w3.org/1998/Math/MathML" display="inline"> <g:mi>C</g:mi> <g:mi>Z</g:mi> </g:math> gate achieves an average fidelity of <i:math xmlns:i="http://www.w3.org/1998/Math/MathML" display="inline"> <i:mn>99.44</i:mn> <i:mo>±</i:mo> <i:mn>0.09</i:mn> <i:mi mathvariant="normal">%</i:mi> </i:math> in a gate duration of 70 ns and that a dispersively driven parametric SWAP-free <l:math xmlns:l="http://www.w3.org/1998/Math/MathML" display="inline"> <l:mi>C</l:mi> <l:mi>Z</l:mi> </l:math> gate attains an average fidelity of <n:math xmlns:n="http://www.w3.org/1998/Math/MathML" display="inline"> <n:mn>99.47</n:mn> <n:mo>±</n:mo> <n:mn>0.07</n:mn> <n:mi mathvariant="normal">%</n:mi> </n:math> in only 30 ns. The fidelity remained above this value for over 8 h and peaked twice with a maximum of <q:math xmlns:q="http://www.w3.org/1998/Math/MathML" display="inline"> <q:mn>99.67</q:mn> <q:mo>±</q:mo> <q:mn>0.14</q:mn> <q:mi mathvariant="normal">%</q:mi> </q:math> . Overall, our parametric approach combines versatility, precision, speed, and high performance in one compact coupler design.

Physical Review AppliedVol. 24(6)
National Institute of Standards and Technology (US), Colorado School of Mines (US), University of Colorado Boulder (US), University of Colorado System (US)
Openalex Percentile: Top 20%
Quantum Computing Algorithms and Architecture
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