2021
DOI: 10.48550/arxiv.2103.07030
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Floating tunable coupler for scalable quantum computing architectures

Eyob A. Sete,
Angela Q. Chen,
Riccardo Manenti
et al.

Abstract: We propose a floating tunable coupler that does not rely on direct qubit-qubit coupling capacitances to achieve the zero-coupling condition. We show that the polarity of the qubit-coupler couplings can be engineered to offset the otherwise constant qubit-qubit coupling and attain the zero-coupling condition when the coupler frequency is above or below the qubit frequencies. We experimentally demonstrate these two operating regimes of the tunable coupler by implementing symmetric and asymmetric configurations o… Show more

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Cited by 5 publications
(5 citation statements)
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“…Beyond the architecture and dispersive regime discussed in this paper, new coupler architecture connecting fixed-frequency floating qubits and new regime were also studied and high-fidelity gates were realized very recently [31,64,65]. Therefore, it would be also interesting to study the interesting physical mechanism behind and explore more possibility.…”
Section: Summary and Perspectivesmentioning
confidence: 91%
“…Beyond the architecture and dispersive regime discussed in this paper, new coupler architecture connecting fixed-frequency floating qubits and new regime were also studied and high-fidelity gates were realized very recently [31,64,65]. Therefore, it would be also interesting to study the interesting physical mechanism behind and explore more possibility.…”
Section: Summary and Perspectivesmentioning
confidence: 91%
“…Cross-Kerr interactions are a source of infidelity for a iSWAP-type gate, as well as in other gate implementations [10][11][12][13][14]47]. In the firstorder RWA Hamiltonian, to cancel the cross-Kerr interaction between the two transmons, we use a coupler with a positive anharmonicity [41] α c > 0, together with α a , α b < 0, which is distinct from using qubits of opposite anharmonicities [10,40], or couplers with negative anharmonicity [14,48]. Equation (20) forms the basis for the optimization of the gate parameters.…”
Section: B Black-box Quantization Approach To the Toy Modelmentioning
confidence: 99%
“…( 2)). However, they may be engineered to have opposite signs as demonstrated in [36,65]. Hence, one can idle the coupler below the qubit frequencies to implement this adiabatic CZ gate scheme by pulsing the coupler uptowards in an almost reversed process.…”
Section: Generalized Control Schemesmentioning
confidence: 99%