Tunable Inductive Coupler for High-Fidelity Gates Between Fluxonium Qubits

Helin Zhang(University of Chicago), Chunyang Ding(University of Chicago), Daniel Weiss(Northwestern University), Ziwen Huang(Northwestern University), Yuwei Ma(University of Science and Technology of China), Charles Guinn(Princeton University), Sara Sussman(Princeton University), Sai Pavan Chitta(Northwestern University), Danyang Chen(Northwestern University), Andrew Houck(Princeton University), Jens Koch(Northwestern University), David Schuster(University of Chicago)
PRX Quantum
May 2, 2024
Cited by 51Open Access
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Abstract

The fluxonium qubit is a promising candidate for quantum computation due to its long coherence times and large anharmonicity. We present a tunable coupler that realizes strong inductive coupling between two heavy-fluxonium qubits, each with approximately <a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline" overflow="scroll"><a:mn>50</a:mn></a:math>-MHz frequencies and approximately <d:math xmlns:d="http://www.w3.org/1998/Math/MathML" display="inline" overflow="scroll"><d:mn>5</d:mn></d:math>-GHz anharmonicities. The coupler enables the qubits to have a large tuning range of <g:math xmlns:g="http://www.w3.org/1998/Math/MathML" display="inline" overflow="scroll"><g:mi>X</g:mi><g:mi>X</g:mi></g:math> coupling strengths (<j:math xmlns:j="http://www.w3.org/1998/Math/MathML" display="inline" overflow="scroll"><j:mo>−</j:mo><j:mn>35</j:mn></j:math> to 75 MHz). The <m:math xmlns:m="http://www.w3.org/1998/Math/MathML" display="inline" overflow="scroll"><m:mi>Z</m:mi><m:mi>Z</m:mi></m:math> coupling strength is <p:math xmlns:p="http://www.w3.org/1998/Math/MathML" display="inline" overflow="scroll"><p:mo>&lt;</p:mo><p:mn>3</p:mn></p:math> kHz across the entire coupler bias range and <s:math xmlns:s="http://www.w3.org/1998/Math/MathML" display="inline" overflow="scroll"><s:mo>&lt;</s:mo><s:mn>100</s:mn></s:math> Hz at the coupler off position. These qualities lead to fast high-fidelity single- and two-qubit gates. By driving at the difference frequency of the two qubits, we realize a <v:math xmlns:v="http://www.w3.org/1998/Math/MathML" display="inline" overflow="scroll"><v:msqrt><v:mi>i</v:mi><v:mrow><v:mstyle mathsize="0.85em"><v:mi>SWAP</v:mi></v:mstyle></v:mrow></v:msqrt></v:math> gate in 258 ns with fidelity 99.72%, and by driving at the sum frequency of the two qubits, we achieve a <z:math xmlns:z="http://www.w3.org/1998/Math/MathML" display="inline" overflow="scroll"><z:msqrt><z:mi>b</z:mi><z:mrow><z:mstyle mathsize="0.85em"><z:mi>SWAP</z:mi></z:mstyle></z:mrow></z:msqrt></z:math> gate in 102 ns with fidelity 99.91%. This latter gate is only five qubit Larmor periods in length. We run cross-entropy benchmarking for over 20 consecutive hours and measure stable gate fidelities, with <db:math xmlns:db="http://www.w3.org/1998/Math/MathML" display="inline" overflow="scroll"><db:msqrt><db:mi>b</db:mi><db:mrow><db:mstyle mathsize="0.85em"><db:mi>SWAP</db:mi></db:mstyle></db:mrow></db:msqrt></db:math> drift (<hb:math xmlns:hb="http://www.w3.org/1998/Math/MathML" display="inline" overflow="scroll"><hb:mn>2</hb:mn><hb:mi>σ</hb:mi></hb:math>) <kb:math xmlns:kb="http://www.w3.org/1998/Math/MathML" display="inline" overflow="scroll"><kb:mo>&lt;</kb:mo><kb:mn>0.02</kb:mn><kb:mi mathvariant="normal">%</kb:mi></kb:math> and <ob:math xmlns:ob="http://www.w3.org/1998/Math/MathML" display="inline" overflow="scroll"><ob:msqrt><ob:mi>i</ob:mi><ob:mrow><ob:mstyle mathsize="0.85em"><ob:mi>SWAP</ob:mi></ob:mstyle></ob:mrow></ob:msqrt></ob:math> drift <sb:math xmlns:sb="http://www.w3.org/1998/Math/MathML" display="inline" overflow="scroll"><sb:mo>&lt;</sb:mo><sb:mn>0.08</sb:mn><sb:mi mathvariant="normal">%</sb:mi></sb:math>. Published by the American Physical Society 2024


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