Transmon ionization (TI) is detrimental to qubit coherence and manipulation. This study explores how TI, triggered by strong microwave pulses, affects microwave single-photon detectors (SPDs) based on a 3D multimode cavity coupled to a transmon qubit. Experimental and numerical investigations reveal that at a critical pump power transmon population suddenly increases, indicating a quantum-to- classical transition. The authors also outline the challenges and potential solutions for increasing the quantum efficiency of SPDs, being crucial for advancing quantum communication and sensing technologies.
Transmon ionization (TI) is detrimental to qubit coherence and manipulation. This study explores how TI, triggered by strong microwave pulses, affects microwave single-photon detectors (SPDs) based on a 3D multimode cavity coupled to a transmon qubit. Experimental and numerical investigations reveal that at a critical pump power transmon population suddenly increases, indicating a quantum-to- classical transition. The authors also outline the challenges and potential solutions for increasing the quantum efficiency of SPDs, being crucial for advancing quantum communication and sensing technologies.
By strongly driving a transmon-resonator system, the transmon qubit may eventually escape from its cosine-shaped potential. This process is called transmon ionization (TI) and known to be detrimental to the qubit coherence and operation. In this work, we investigate the onset of TI in an irreversible, parametrically-driven, frequency conversion process in a system consisting of a superconducting 3D-cavity coupled to a fixed-frequency transmon qubit. Above a critical pump power we find a sudden increase in the transmon population. Using Renyi entropy, Floquet modes, and Husimi Q functions, we infer that this abrupt change can be attributed to a quantum-to-classical phase transition. Furthermore, in the context of the single-photon detection, we measure a TI-uncorrected detection efficiency of up to 86% and estimate a TI-corrected value of up to 78% by exploiting the irreversible frequency conversion. Our numerical simulations suggest that increasing the detuning between the pump and qubit frequencies and increasing the qubit anharmonicity can suppress the TI impact. Our findings highlight the general importance of the TI process when operating coupled qubit-cavity systems.
The detection of single microwave photons is becoming a cornerstone of fundamental experiments in circuit quantum electrodynamics and quantum sensing. Experiments in cavity quantum electrodynamics, photon-mediated entanglement, dark-matter axion searches and quantum thermodynamics increasingly rely on single-photon sensitivity. Current technologies exploit superconducting devices, including Josephson parametric detectors, and transmon-based non-demolition counters for dark-matter haloscopes. Hybrid double quantum dot-Josephson systems reach interesting levels of efficiency, while current-biased Josephson junctions show potential for near-quantumlimited resolution. Despite impressive progress, challenges remain in reducing dark counts, improving reset speed, and scaling for multiplexed arrays. Continued advances in superconducting materials, qubit coherence, and hybrid semiconductor-superconductor designs promise to extend detection efficiency and bandwidth. These developments are poised to enable the next generation of quantum-enabled experiments, from foundational tests in quantum optics to searches for new physics.
Detecting an itinerant microwave photon with high efficiency is an outstanding problem in quantum optics at microwave frequencies and in the fundamental quantum mechanics experimental toolbox. This subject has attracted a lot of attention and there are growing number of excellent experimental demonstrations and theoretical proposals towards this aim. However, due to the extremely low energy of microwave quanta, efficiently detecting a propagating microwave photon in a non-absorbing manner is still an unresolved challenge and it is the focus of the major part of this thesis. Motivated by a recent experiment that shows a superconducting artificial atom (a transmon) in a one-dimensional microwave transmission line exhibits gigantic cross-Kerr nonlinearities, 1000 times larger than in comparable optical systems, I investigate the possibility of detection single microwave photons using a transmon induced cross-Kerr-like interaction between two microwave fields. The photon number in one field is inferred through the measurement of the displacement of the other field. The first project on this subject is to investigate the feasibility of detecting a single microwave photon with signal-to-noise ratio (SNR) greater than unity using a three-level approximation for the transmon in an open transmission line, due to the saturation of transmon response to the probe intensity. After that, an improved scheme was proposed to overcome the limitations in the preceding work. By using a cavity probe field the signal photon induced probe displacement is strongly enhanced. Further additional transmon-cavity units can be cascaded to further improve the detection efficiency. It is shown that with only two transmons the distinguishability to resolve a single-photon state from the vacuum is up to 90%. One advantage of this photon detection scheme is that it does not rely on the absorption of single microwave photons, which enables repeated measurements and further applications. Moreover, I also show how the measurement diminishes coherence in the photon number basis thereby illustrating a fundamental principle of quantum measurement: the higher the measurement efficiency, the greater is the decoherence. Apart from the investigation on the single microwave photon detection, this thesis also studies nonlinear dynamics of a hybrid coupled-resonator and opto-mechanical system. It is shown that the saddle-node bifurcation and the Hopf bifurcation appear in the system, which leads to bistability and limit cycle dynamics of the mechanical position and the output light intensity. More importantly, the opto-mechanical nonlinearity dramatically changes the transparency window of the coupled resonator induced transparency (CRIT) and based on the narrow and bistable CRIT transparency window, the proposed system is shown to be a good platform for the weak impulsive force detection with a good sensitivity.
Abstract We present a detailed study of a microwave single-photon source utilizing a transmon qubit asymmetrically coupled to two transmission lines: a weakly coupled drive line and a strongly coupled emission line. Our design allows for the generation of single photons in the microwave regime, which are essential for quantum communication, computing, and sensing applications. In addition to single-photon generation, the same design functions as a power sensor and enables precise measurement of the system’s attenuation. This dual functionality allows us to calibrate the noise of our amplification chain. This enables a self-calibrated architecture in which the same device acts simultaneously as the photon source and as a reference standard, eliminating the need for external tones or calibrated inputs. With this calibration we reconstruct the density matrix of the emitted photon state, for which we achieve a fidelity of 61.4% and measure a second-order correlation function of g ( 2 ) ( 0 ) = 0.06 − 0.06 + 0.45 , indicating quantum nature and single-photon characteristics. These results confirm generation of single photons and demonstrate the potential of transmon qubits in advancing quantum technologies in the microwave domain.
We develop a compact transmon emitter/detector (TED) superconducting circuit and demonstrate its dual functionality as a single-photon source and detector. In our setup, photons emitted by a source TED are transmitted via a meter-long coaxial cable, routed through a circulator, and captured by a measurement TED. Both TED modules operate with nominally identical parameters, highlighting the flexibility of this novel architecture. Furthermore, we introduce an efficient microwave photon detection scheme tailored to the TED. Using this setup, we detect 60% of the emitted Fock state photons and infer a 95% detection efficiency at the input of the measurement TED, which we calibrate against coherent state measurements. The reset and photon emission/detection processes each require approximately 2μs, yielding a minimum protocol duration of 4μs as constrained by our chosen TED parameters. Ultimately, the TED demonstrates a new use case for the recently developed double transmon coupler (DTC): a compact, drop-in, tunable, and transition-selective link between a coherent data transmon and a waveguide. Circuits like the TED will play a vital role in quantum information processing by facilitating unconditional fast reset, enabling microwave photon metrology, and serving as nascent quantum communication interfaces (QCIs). QCIs mediate entanglement distribution between quantum processing units (QPUs) within a cryostat or interface with microwave-to-optical transducers for long-range quantum networking.
We present the observation of photon number splitting (PNS) in a superconducting transmon qubit with different microwave photon sources. Such PNS is not limited to the lower energy levels and can also be observed in the higher energy levels of a superconducting transmon qubit. The sideband transition, Autler-Townes splitting, and the absence of PNS are demonstrated under certain conditions. Furthermore, we investigate the PNS induced by the nonclassical microwave photons emitted from a dual-mode Josephson parametric amplifier, which can operate in either the single mode or dual mode. The evolution from the dual-mode squeezing to the self-oscillation light emission is demonstrated. Our results provide a useful reference for future investigations, such as the exploration of more nonlinear effects in strongly driven circuit QED systems, the manipulation of quantum states, and the characterization of the quantum microwave source by utilizing PNS.