Nature Communications · 2016 · 196 citations · 33 references
Natural SciencesElectrical EngineeringPhysicsPhotonicsQuantum ComputingQuantum MechanicsQuantum BitsQuantum ControlQuantum MeasurementQuantum OpticsSuperconducting QubitsMicrowave Detector DesignPhoton DetectorsPhoton EnergyQuantum PhotonicsQuantum Signal ProcessingSensingSingle-photon DetectionSingle-photon Detectors
Single‑photon detection is essential for quantum‑optics experiments, but microwave photons are 10^4–10^5 times less energetic than optical ones, making efficient detection extremely difficult. This work demonstrates the detection of a single microwave photon propagating through a waveguide. The detector employs an impedance‑matched artificial Λ system formed by the dressed states of a driven superconducting qubit coupled to a microwave resonator, where each photon deterministically drives a Raman transition that excites the qubit and produces a discrete dispersive readout click. The device achieves a single‑photon detection efficiency of 0.66 ± 0.06, a dark‑count probability of 0.014 ± 0.001, and a reset time of ≈400 ns, enabling applications in quantum sensing, communication, and information processing.
Abstract Single-photon detection is a requisite technique in quantum-optics experiments in both the optical and the microwave domains. However, the energy of microwave quanta are four to five orders of magnitude less than their optical counterpart, making the efficient detection of single microwave photons extremely challenging. Here we demonstrate the detection of a single microwave photon propagating through a waveguide. The detector is implemented with an impedance-matched artificial Λ system comprising the dressed states of a driven superconducting qubit coupled to a microwave resonator. Each signal photon deterministically induces a Raman transition in the Λ system and excites the qubit. The subsequent dispersive readout of the qubit produces a discrete ‘click’. We attain a high single-photon-detection efficiency of 0.66±0.06 with a low dark-count probability of 0.014±0.001 and a reset time of ∼400 ns. This detector can be exploited for various applications in quantum sensing, quantum communication and quantum information processing.
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