Superconducting quantum circuits are one of the leading quantum computing platforms. To advance superconducting quantum computing to a point of practical importance, it is critical to identify and address material imperfections that lead to decoherence. Here, we use terahertz scanning near-field optical microscopy to probe the local dielectric properties and carrier concentrations of wet-etched aluminum resonators on silicon, one of the most characteristic components of the superconducting quantum processors. Using a recently developed vector calibration technique, we extract the THz permittivity from spectroscopy in proximity to the microwave feedline. Fitting the extracted permittivity to the Drude model, we find that silicon in the etched channel has a carrier concentration greater than buffer oxide etched silicon and we explore post-processing methods to reduce the carrier concentrations. Our results show that near-field THz investigations can be used to quantitatively evaluate and identify inhomogeneities in quantum devices.
Superconducting quantum circuits are one of the leading quantum computing platforms. To advance superconducting quantum computing to a point of practical importance, it is critical to identify and address material imperfections that lead to decoherence. Here, we use terahertz scanning near-field optical microscopy to probe the local dielectric properties and carrier concentrations of wet-etched aluminum resonators on silicon, one of the most characteristic components of the superconducting quantum processors. Using a recently developed vector calibration technique, we extract the THz permittivity from spectroscopy in proximity to the microwave feedline. Fitting the extracted permittivity to the Drude model, we find that silicon in the etched channel has a carrier concentration greater than buffer oxide etched silicon and we explore post-processing methods to reduce the carrier concentrations. Our results show that near-field THz investigations can be used to quantitatively evaluate and identify inhomogeneities in quantum devices.
We systematically investigate the influence of the fabrication process on dielectric loss in aluminum-on-silicon superconducting coplanar waveguide resonators with internal quality factors (Qi) of about one million at the single-photon level. These devices are essential components in superconducting quantum processors; they also serve as proxies for understanding the energy loss of superconducting qubits. By systematically varying several fabrication steps, we identify the relative importance of reducing loss at the substrate–metal and substrate–air interfaces. We find that it is essential to clean the silicon substrate in hydrogen fluoride (HF) prior to aluminum deposition. A post-fabrication removal of the oxides on the surface of the silicon substrate and the aluminum film by immersion in HF further improves the Qi. We observe a small, but noticeable, adverse effect on the loss by omitting either standard cleaning (SC1), pre-deposition heating of the substrate to 300 °C, or in situ post-deposition oxidation of the film’s top surface. We find no improvement due to excessive pumping meant to reach a background pressure below 6 × 10−8 mbar. We correlate the measured loss with microscopic properties of the substrate–metal interface through characterization with x-ray photoelectron spectroscopy, time-of-flight secondary ion mass spectrometry, transmission electron microscopy, energy-dispersive x-ray spectroscopy, and atomic force microscopy.
Correlating superconducting qubit performance with advanced materials analysis is a key strategy for improving coherence. Existing diagnostics for key properties, such as dielectric loss, structural discontinuity, and interface heterogeneity, often rely on destructive electron microscopy or low-throughput millikelvin measurements. Here, we demonstrate noninvasive terahertz (THz) nano-imaging/spectroscopy of encapsulated niobium transmon qubits as a high-throughput proxy for performance evaluation. We identify large variations in sidewall near-field signals, implicating sidewall loss and discontinuity as major coherence limiters, and also use THz hyperspectral line scans to probe dielectric responses and field participation at Al junction interfaces.
Abstract Dielectric losses are one of the key factors limiting the coherence of superconducting qubits. The impact of materials and fabrication steps on dielectric losses can be evaluated using coplanar waveguide (CPW) microwave resonators. Here, we report on superconducting CPW microwave resonators with internal quality factors systematically exceeding 5 × 106 at high powers and 2 × 106 (with the best value of 4.4 × 106) at low power. Such performance is demonstrated for 100-nm-thick aluminum resonators with 7–10.5 um center trace on high-resistivity silicon substrates commonly used in Josephson-junction based quantum circuit. We investigate internal quality factors of the resonators with both dry and wet aluminum etching, as well as deep and isotropic reactive ion etching of silicon substrate. Josephson junction compatible CPW resonators fabrication process with both airbridges and silicon substrate etching is proposed. Finally, we demonstrate the effect of airbridges’ positions and extra process steps on the overall dielectric losses. The best quality factors are obtained for the wet etched aluminum resonators and isotropically removed substrate with the proposed ultrasonic metal edge microcutting.
Quantum sensing and computation can be realized with superconducting microwave circuits. Qubits are engineered quantum systems of capacitors and inductors with non-linear Josephson junctions. They operate in the single-excitation quantum regime, photons of 27μeV at 6.5 GHz. Quantum coherence is fundamentally limited by materials defects, in particular atomic-scale parasitic two-level systems (TLS) in amorphous dielectrics at circuit interfaces.[1] The electric fields driving oscillating charges in quantum circuits resonantly couple to TLS, producing phase noise and dissipation. We use coplanar niobium-on-silicon superconducting resonators to probe decoherence in quantum circuits. By selectively modifying interface dielectrics, we show that most TLS losses come from the silicon surface oxide, and most non-TLS losses are distributed throughout the niobium surface oxide. Through post-fabrication interface modification we reduced TLS losses by 85% and non-TLS losses by 72%, obtaining record single-photon resonator quality factors above 5 million and approaching a regime where non-TLS losses are dominant. [1]Müller, C., Cole, J. H. & Lisenfeld, J. Towards understanding two-level-systems in amorphous solids: insights from quantum circuits. Rep. Prog. Phys. 82, 124501 (2019)
Superconducting resonator systems, including a superconducting qubit, require exceptional coherence and longevity lifetime performance. However, these systems have been impeded by dielectric loss and quasiparticle loss, many of which have been caused by the materials imperfection [1]. In this work, we report a comparative scanning transmission electron microscopy (S/TEM) investigation of the impacts of wet and dry etching on superconducting Tantalum (Ta) films. This work has been sparked by the critical importance of superconducting resonators in a wide range of quantum technological applications, which necessitates optimizing their fabrications to improve the performance of various quantum devices and communication systems [2]. The primary objective of this work is to understand the morphology, substrate crystallinity degradation, chemical segregation, and strain of etched Ta films, as well as the characteristics of the oxidized sidewalls that can influence the performance and homogeneity of the superconducting device. In the pursuit of deeper insights, advanced characterization techniques such as atomic-resolution STEM imaging, electron energy loss spectroscopy (EELS) chemical mapping, and 4-dimensional STEM (4D STEM) strain mapping were employed. The key findings of this work are the significant variations in sidewall morphology, chemical composition, and strain fields depending on the type of etching employed (wet or dry). The findings suggest that sidewall formation induces localized strain fields in proximity to amorphized oxidation layers of the superconducting resonator sidewalls, which potentially impacting the coherence and homogeneity of the superconducting quantum devices [3]. This study, therefore, emphasizes the need to optimize the morphology of the sidewall to minimize local strain field generation. Additionally, the research underscores the importance of precise and meticulous fabrication in the construction of quantum devices, emphasizing the need for a chemically robust and uniform coating process to protect the resonator film from oxidation and wet etchants without affecting the operation of the superconducting device. These insights are crucial for advancing the performance and coherence of superconducting qubits, ultimately contributing to the optimization of quantum devices and the progress of quantum technologies and high-frequency communication systems [4]. Top-view schematics of Ta superconducting resonators at (a) zoom-out view and (b) zoom-in view. Cross-sectional HAADF STEM images of (c) dry- and (d) wet-etched Ta film on sapphire substrate. These images show the overall dimensions and morphologies of the resonators. The BF STEM images, εxx, εzz, εxz, and ωxz mapping results were virtually reconstructed from 4D STEM for the (a) dry- and (b) wet-etched samples, respectively. The positive (negative) value is represented by the color red (blue) in the colorbar. Lattice elongation (shrinkage), is represented by positive (negative) values in εxx and εzz. Lattice shearing, which has a positive value in εxz, is defined as distortion from the top to the right and the bottom to the left of the lattice. The Ta lattice rotates counterclockwise (clockwise) represented by positive (negative) numbers in ωxz.