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March 6, 2026Journal of Low Temperature Physics0 citationsOpen Access

Scanning Tunneling Spectroscopy of Superconducting Nitridized Aluminum Thin Films

JMJose Antonio MorenoPTPablo García TalaveraATAlba Torras-Coloma

Key Points

  • This research aims to explore the microscopic properties of nitridized aluminum (NitrAl) and its potential for quantum circuit applications.
  • Utilized scanning tunneling microscopy (STM) to analyze nitridized aluminum thin films.
  • Measured superconducting density of states and resistivity at room temperature.
  • Analyzed spatial variation of superconducting gap values using STM.
  • Found that the in-gap density of states is zero up to approximately 250 μeV.
  • Detected distribution of superconducting gap values at around 360 μeV, close to BCS predictions.
  • Observed spatial variation of the superconducting gap by about 10% across different sample regions.

Abstract

Abstract Nitride-based superconductors represent a family of superconducting thin film materials displaying higher quality than their corresponding bare superconductor when used in devices for applications such as cosmic radiation sensing. In recent times, niobium-based and titanium-based nitrides were used to improve the quality of superconducting devices in quantum technology applications. Recently, nitridized aluminum (NitrAl) has been found to display higher critical temperatures and enhanced resilience to magnetic fields compared to those of Al, making it a new interesting candidate for superconducting quantum circuit applications. However, the microscopic properties of NitrAl remain highly unexplored. Here, we use scanning tunneling microscope (STM) to measure the superconducting density of states of a thin film sample of nitridized aluminum (NitrAl), with a room temperature resistivity between pure Al and fully insulating aluminum nitride. We show that the in-gap density of states is zero up to about =250~ eV ħ ω = 250 μ eV and that there is a distribution of values of the superconducting gap around ₀=360~ eV Δ 0 = 360 μ eV, close to the BCS expectation =1. 76 k₁T₂ Δ = 1. 76 k B T c. We also find varying superconducting gap values at the nanometer scale, by approximately 10%, when probing different regions of the sample. These results suggest a gap which is larger than the one of pure Al and is spatially more homogeneous than the superconducting gap values often found in thin films. Our work demonstrates that STM is as a powerful tool to screen materials for quantum devices through the measurement of the spatial dependence of the superconducting density of states.

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Cite This Study

Moreno et al. (2026) studied this question.

synapsesocial.com/papers/69aa6f3c531e4c4a9ff59412https://doi.org/10.1007/s10909-026-03390-y
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