The integration, scale-up, and multiplexing arrays of superconducting qubits in quantum circuits are the main challenges of superconducting quantum technology. Here we experimentally investigate the solid-state qubit multiplexing readout scheme, containing coplanar quarter-wavelength resonators coupled with a planar Xmon-type qubit, connected to a common coplanar transmission line. We find that the qubit energy spectrum is modified in the presence of an additional exciting signal at the fundamental frequency of the neighboring resonators. We attribute the origin of this effect to the electromagnetic field propagating through the common ground plane, which changes the qubit’s characteristics. Our finding may be useful for the development of scalable superconducting quantum integrated circuits with arrays of multiplexed or coupled qubits for applications in superconducting quantum processing and computing.

We present a method for in situ temperature measurement of superconducting quantum circuits, by using the first three levels of a transmon device to which we apply a sequence of π gates. Our approach employs projective dispersive readout and utilizes the basic properties of the density matrix associated with thermal states. This method works with an averaging readout scheme and does not require a single-shot readout setup. We validate this protocol by performing thermometry in the range of 50–200 mK, corresponding to a range of residual populations 1%–20% for the first excited state and 0.02%–3% for the second excited state.

The operating principle of traveling-wave parametric amplifiers is typically understood in terms of the standard coupled mode theory, which describes the evolution of forward propagating waves without any reflections, i.e., for perfect impedance matching. However, in practice, superconducting microwave amplifiers are unmatched nonlinear finite-length devices, where the reflecting waves undergo complex parametric processes, not described by the standard coupled mode theory. Here, we present an analytical solution for the TWPA gain, which includes the interaction of reflected waves. These reflections result in corrections to the well-known results of the standard coupled mode theory, which are obtained for both three-wave and four-wave mixing processes. Due to these reflections, the gain is enhanced and unwanted nonlinear phase modulations are suppressed. Predictions of the model are experimentally demonstrated on two types of unmatched TWPA, based on coplanar waveguides with a central wire consisting of (i) a high kinetic inductance superconductor, and (ii) an array of 2000 Josephson junctions.

Josephson tunnel junctions represent a key element in superconducting electronics and quantum circuits. For many years, shadow evaporation by means of Dolan-type bridges has been the state-of-the-art for deep sub- micrometer sized structures. Increasing demand in the number of Josephson junctions, e.g., in qubit circuits and travelling wave parametric amplifiers, requests for a wafer-scale fabrication process with precise control of junction parameters and have led to an advanced lift-off technique called Manhattan-type junction technology in recent years. Herein, we report on the development of a 100 mm wafer-scale fabrication technology for deep sub-micrometer sized Al Josephson junctions with linear dimensions down to 180 nm. The critical current I_C of the junctions ranges from about 10 to 120 nA scaling with their linear dimensions. Low temperature transport measurements as well as room-temperature characterization has been used for I_C and process homogeneity determination of series arrays of up to 50 Josephson junctions. We discuss technology parameters such as yield, on-chip and on-wafer reproducibility of the junction's critical currents as well as main process limitations. Moreover, we present experimental results on the characterization of first transmon-type qubits fabricated using this technology.

In the upcoming decades quantum technologies, especially quantum computation, will have a strong influence on industrial, technological, economic, and social progress and are, therefore, considered to be one of the key technologies. The fundamental building blocks for quantum computation are quantum bits (qubits). The superconducting platform offers one of the most promising implementations due to its monolithic character and potential for scalability. Present research around the world primarily focusses on scaling up the number of qubits, so reliable wafer-scale fabrication technologies are mandatory. In this paper, we present our recent developments on wafer-scale fabrication of superconducting quantum circuits including Josephson junctions by the Manhattan-type technology. We discuss fabrication parameters as well as electrical characterization. For arrays out of 50 Josephson junctions with structure dimensions of 200 nm x 200 nm, we achieve a critical current standard deviation of approx. 3 % on-chip and 7 % on-wafer. We also show first measurement results of so fabricated transmon-type qubits with relaxation and decoherence times of T ₁ = 12.5 μs and T ₂ = 15.0 μs, respectively. With an increasing number of superconducting qubits and, thus, their input and read-out lines, new challenges arise: Crosstalk between qubits, unwanted modes in the qubit environment, and required interconnections. One way to counteract is the implementation of low inductance connections across coplanar waveguides. This can be realized by aluminum air bridges. In this paper we discuss the air bridges' fabrication parameters and the impact on the integrated circuits' elements, e.g. Josephson junctions. We show electrical and superconducting measurements with critical temperatures and critical currents of T _c > 1.0 K and I _c > 0.6 mA, respectively.

We measured the relaxation and decoherence rates of a superconducting transmon qubit in a resonator-free setting. In our experiments, the qubit is coupled to an open coplanar waveguide such that the transmission of microwaves through this line depends on the qubit's state. To determine the occupation of the first excited qubit energy level, we introduced a two-pulse technique. The first applied pulse, at a frequency close to the eigenfrequency of the qubit, serves to excite the qubit. A second pulse is then used for probing the transition between the first and second excited energy levels. Utilizing this measurement technique allowed for the reconstruction of the relaxation dynamics and Rabi oscillations. Furthermore, we demonstrate the consistency between the extracted parameters and the corresponding estimations from frequency-domain measurements.