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Sensors

Population-Based Discrimination of Classical and Few-Photon Microwave Fields with a Flux-Tunable Transmon Qudit

A.V. Pashchenko, Olga V. Tikhonova, Irina A Solovykh, Соловьев Игорь Иванович, Maxim V Tereshonok, N. V. Klenov, Dmitry S. Yakovlev

Published Oct 15, 2026• 0 citations
Publisher

Abstract

Interactions between few-photon microwave fields and superconducting artificial atoms provide a method to study photon statistics and manipulate quantum states for photonic quantum information processing. Superconducting transmons couple to microwave fields through an anharmonic ladder of energy levels, producing a response beyond the two-level description. Here, we propose and analyze a detector based on a flux-tunable transmon qudit in circuit quantum electrodynamics. Within a Kerr-type model, we calculate its population response to classical-field excitation and quantized Fock and coherent states. In the four-photon example, a selected detuning produces periodic, nearly complete transfer to the fourth transmon level for a Fock input, while a coherent input of equal mean energy gives a population of approximately 0.2 at the same interaction time. In the linear regime, we derive a target-population bound for classical inputs. From single-tone and two-tone spectroscopy, analyzed using the cosine transmon Hamiltonian, we extract circuit parameters and resolve higher transitions. Ramsey interferometry characterizes dephasing on the fundamental transition. We propose a detection protocol combining flux-selected interaction with dispersive population readout. Our results establish a population-based framework for microwave-state discrimination using a superconducting artificial atom.

DOI
10.3390/s26206538

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Interactions between few-photon microwave fields and superconducting artificial atoms provide a method to study photon statistics and manipulate quantum states for photonic quantum information processing. Superconducting transmons couple to microwave fields through an anharmonic ladder of energy levels, producing a response beyond the two-level description. Here, we propose and analyze a detector based on a flux-tunable transmon qudit in circuit quantum electrodynamics. Within a Kerr-type model, we calculate its population response to classical-field excitation and quantized Fock and coherent states. In the four-photon example, a selected detuning produces periodic, nearly complete transfer to the fourth transmon level for a Fock input, while a coherent input of equal mean energy gives a population of approximately 0.2 at the same interaction time. In the linear regime, we derive a target-population bound for classical inputs. From single-tone and two-tone spectroscopy, analyzed using the cosine transmon Hamiltonian, we extract circuit parameters and resolve higher transitions. Ramsey interferometry characterizes dephasing on the fundamental transition. We propose a detection protocol combining flux-selected interaction with dispersive population readout. Our results establish a population-based framework for microwave-state discrimination using a superconducting artificial atom.
We investigate the dynamics of superconducting transmon-based artificial atom under the influence of quantum and classical microwave fields, revealing fundamental differences in their interaction mechanisms. A classical field, acting as an unlimited energy reservoir, sequentially populates the transmon levels, resulting in a Poissonian distribution of level populations. In contrast, a quantum field with its discrete structure and finite photon number exhibits oscillatory population dynamics with a binomial probability distribution, enabling the transfer of quantum statistics between the field and the atom. In the strong coupling regime and with optimal frequency detuning, the quantum field demonstrates the ability to selectively and efficiently populate specific transmon levels, a feature inaccessible to its classical counterpart. These distinctions highlight the potential of transmon qudits as quantum interfaces and detectors of non-classical microwave states in distributed quantum computing architectures.
PhD Thesis: Superconducting circuit quantum electrodynamics (QED) has developed into a powerful platform for studying the interaction between matter and different states of light. In this context, superconducting quantum bits (qubits) act as artificial atoms interacting with quantized modes of the electromagnetic field. The field can be trapped in superconducting microwave resonators or propagating in transmission lines. In this thesis, we particularly study circuit QED systems where microwave fields are coupled with superconducting flux and transmon qubits. We optimize the coherence properties of the resonators, by analyzing loss mechanisms at excitation powers of approximately one photon on average. We find that two-level fluctuators associated with oxide layers at substrate and metal surfaces and metal-metal interfaces represent the predominant loss channel. Furthermore, we show how broadband thermal photon fields influence the relaxation and dephasing properties of a superconducting transmon qubit. To this end, we study several second-order loss channels of the transmon qubit and find that the broadband fields introduce a larger decay rate than expected from the Purcell filter defined by the resonator. Additionally, we show that qubit dephasing at the flux-insensitive point as well as low-frequency parameter fluctuations can be enhanced by thermal fields. Finally, we study how artificial atoms react to changes in inherent properties of the light fields. We perform a detailed analysis of the photon statistics of thermal fields using their relation to the qubits coherence properties. We quantitatively recover the expected n2 + nn^{2}\,{+}\,nn2+n-law for the photon number variance and confirm this result by direct correlation measurements. We then show a novel technique for the in-situ conversion of the interaction parity in light-matter interaction. To this end, we couple spatially controlled microwave fields to a flux qubit with two degrees of freedom.
In the circuit quantum electrodynamics architecture, both the resonance frequency and the coupling of superconducting qubits to microwave field modes can be controlled via external electric and magnetic fields to explore qubit-photon dynamics in a wide parameter range. Here, we experimentally demonstrate and analyze a scheme for tuning the coupling between a transmon qubit and a microwave resonator using a single coherent drive tone. We treat the transmon as a three-level system, with the qubit subspace defined by the ground and the second excited states. If the drive frequency matches the difference between the resonator and the qubit frequencies, a Jaynes-Cummings-type interaction is induced, which is tunable in both amplitude and phase. We show that coupling strengths of about 10 MHz can be achieved in our setup, limited only by the anharmonicity of the transmon qubit. This scheme has been successfully used to generate microwave photons with a controlled temporal shape [M. Pechal et al., Phys. Rev. X 4, 041010 (2014)] and can be directly implemented with superconducting quantum devices featuring larger anharmonicity for higher coupling strengths.
Using circuit QED, we consider the measurement of a superconducting transmon qubit via a coupled microwave resonator. For ideally dispersive coupling, ringing up the resonator produces coherent states with frequencies matched to transmon energy states. Realistic coupling is not ideally dispersive, however, so transmon-resonator energy levels hybridize into joint eigenstate ladders of the Jaynes--Cummings type. Previous work has shown that ringing up the resonator approximately respects this ladder structure to produce a coherent state in the eigenbasis (a dressed coherent state). We numerically investigate the validity of this coherent-state approximation to find two primary deviations. First, resonator ring-up leaks small stray populations into eigenstate ladders corresponding to different transmon states. Second, within an eigenstate ladder the transmon nonlinearity shears the coherent state as it evolves. We then show that the next natural approximation for this sheared state in the eigenbasis is a dressed squeezed state and derive simple evolution equations for such states by using a hybrid phase--Fock-space description.
Superconducting quantum bits (qubits) are a leading candidate towards realizing a processor that is able to outperform existing classical computers at select tasks. One particular qubit architecture, the transmon, boasts long coherence times compared to required gate lengths and flexibility with respect to circuit couplings as these 'artificial atoms' are photolithographically defined. These attributes allow qubits to be leveraged for other tasks as well — such as efficiently detecting itinerant microwave photons. Such a device may prove useful for remote entanglement protocols, quantum optics experiments in the microwave regime, and as a detector for low-mass dark matter.Through a blend of circuit quantum electrodynamics (cQED) and waveguide quantum electrodynamics (wQED) theories, high detector performance was achieved even when the photon arrival time was not known. Utilizing an ensemble (N = 4) of identical transmon absorbers, photon mediated interactions along a common waveguide enable absorbed itinerant photons to be trapped for longer than the inverse of the bandwidth of an individual qubit. This extended trapping time allows for sufficient integration of the dispersively shifted readout resonator to resolve deviations from vacuum with high fidelity.
The interaction-free measurement is a fundamental quantum effect whereby the presence of a photosensitive object is determined without irreversible photon absorption. Here we propose the concept of coherent interaction-free detection and demonstrate it experimentally using a three-level superconducting transmon circuit. In contrast to standard interaction-free measurement setups, where the dynamics involves a series of projection operations, our protocol employs a fully coherent evolution that results, surprisingly, in a higher probability of success. We show that it is possible to ascertain the presence of a microwave pulse resonant with the second transition of the transmon, while at the same time avoid exciting the device onto the third level. Experimentally, this is done by using a series of Ramsey microwave pulses coupled into the first transition and monitoring the ground-state population.