Abstract

We demonstrate an on-demand source of microwave single photons with 71–99% intrinsic quantum efficiency. The source is narrowband (300 kHz) and tuneable over a 600 MHz range around 5.2 GHz. Such a device is an important element in numerous quantum technologies and applications. The device consists of a superconducting transmon qubit coupled to the open end of a transmission line. A π-pulse excites the qubit, which subsequently rapidly emits a single photon into the transmission line. A cancellation pulse then suppresses the reflected π-pulse by 33.5 dB, resulting in 0.005 photons leaking into the photon emission channel. We verify strong antibunching of the emitted photon field and determine its Wigner function. Non-radiative decay and 1/f flux noise both affect the quantum efficiency. We also study the device stability over time and identify uncorrelated discrete jumps of the pure dephasing rate at different qubit frequencies on a time scale of hours, which we attribute to independent two-level system defects in the device dielectrics, dispersively coupled to the qubit. Our single-photon source with only one input port is more compact and scalable compared to standard implementations.

Highlights

  • The single photon—the fundamental excitation of the electromagnetic field—plays a key role in quantum physics and can find practical application in quantum sensing[1], communication[2], and computing[3,4,5]

  • Our device consists of a magnetic-flux-tunable Xmon-type transmon qubit, capacitively coupled to the open end of a onedimensional coplanar-waveguide transmission line

  • We demonstrate a method to implement a frequency-tunable single-photon source by using a superconducting qubit

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Summary

Introduction

The single photon—the fundamental excitation of the electromagnetic field—plays a key role in quantum physics and can find practical application in quantum sensing[1], communication[2], and computing[3,4,5]. In the microwave domain, the much smaller photon energy introduces many constrains for the realization of singlephoton sources; for instance, operation at millikelvin temperatures is necessary to avoid thermal generation of photons. Narrowband microwave single photons are essential for precise interactions with circuits exhibiting a shaped energy structure, such as coplanar resonators[9], three-dimensional cavities[10], and acoustic-wave resonators[11,12], which can be used as quantum memories. Superconducting quantum circuits are suitable for the implementation of on-demand microwave photon sources. The first method is based on a qubit coupled to a resonator[13,14,15], where the source bandwidth is limited by the linewidth of the resonator. In refs. 16–18, single photons are generated due to inelastic

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