Abstract

Circuit quantum electrodynamics (QED) employs superconducting microwave resonators as quantum buses. In circuit QED with semiconductor quantum-dot-based qubits, increasing the resonator impedance is desirable as it enhances the coupling to the typically small charge dipole moment of these qubits. However, the gate electrodes necessary to form quantum dots in the vicinity of a resonator inadvertently lead to a parasitic port through which microwave photons can leak, thereby reducing the quality factor of the resonator. This is particularly the case for high-impedance resonators, as the ratio of their total capacitance over the parasitic port capacitance is smaller, leading to larger microwave leakage than for 50-$\Omega$ resonators. Here, we introduce an implementation of on-chip filters to suppress the microwave leakage. The filters comprise a high-kinetic-inductance nanowire inductor and a thin-film capacitor. The filter has a small footprint and can be placed close to the resonator, confining microwaves to a small area of the chip. The inductance and capacitance of the filter elements can be varied over a wider range of values than their typical spiral inductor and interdigitated capacitor counterparts. We demonstrate that the total linewidth of a 6.4 GHz and approximately 3-k$\Omega$ resonator can be improved down to 540 kHz using these filters.

Highlights

  • Superconducting microwave resonators enable a rich variety of quantum-mechanical phenomena in micro- and nanodevices at cryogenic temperatures, known as circuit quantum electrodynamics (QED)

  • We develop on-chip filters, consisting of a high-kinetic-inductance nanowire serving as a compact inductor and a small thin-film capacitor, to mitigate leakage from a high-impedance half-wave resonator with silicon double quantum dots (DQDs) at each end

  • We verify that the devices measured in our 3He system have similar linewidths, both the good and poor ones, to the ones obtained in our dilution refrigerator setup with all gate lines connected individually to real instruments

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Summary

Introduction

Superconducting microwave resonators enable a rich variety of quantum-mechanical phenomena in micro- and nanodevices at cryogenic temperatures, known as circuit quantum electrodynamics (QED). QD systems typically have a small charge dipole moment, while the coupling to spin qubits is achieved through spin-charge hybridization [16,17]. This results in a relatively weak coupling to the resonator mode. High-impedance resonators are desirable, since their small capacitance produces large electric fields that enhance this coupling [9,10,18,19]. The same physical advantages of high-impedance resonators have

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