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arxiv: 2601.21953 · v1 · submitted 2026-01-29 · ❄️ cond-mat.mtrl-sci · quant-ph

Fabrication effects on Niobium oxidation and surface contamination in Niobium-metal bilayers using X-ray photoelectron spectroscopy

Pith reviewed 2026-05-16 09:26 UTC · model grok-4.3

classification ❄️ cond-mat.mtrl-sci quant-ph
keywords niobiumoxidationcapping layersXPSsuperconducting resonatorsfabrication processessurface contamination
0
0 comments X

The pith

XPS screens 17 metal caps to identify which best block oxygen diffusion into niobium during fabrication.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper applies X-ray photoelectron spectroscopy to measure surface oxidation and contamination on niobium films capped with 17 different metals. It tracks how standard steps such as annealing, resist stripping, and acid cleaning change those surfaces. Resilient caps are chosen on the basis of the XPS data and then built into microwave resonators to test actual performance. A sympathetic reader would care because surface oxides are a major source of dielectric loss in superconducting circuits, and a fast screening method could shorten the path to lower-loss devices.

Core claim

XPS functions as a non-destructive probe that quantifies oxygen uptake and contaminant levels in niobium-metal bilayers after each fabrication process, allowing the authors to rank the 17 caps by protective effectiveness and to select a subset whose microwave resonators show improved characteristics.

What carries the argument

X-ray photoelectron spectroscopy measurements of surface oxygen concentration and chemical state in niobium capped by different metals, used to rank resistance to diffusion under annealing, stripping, and cleaning.

If this is right

  • Capping layers that keep oxygen low after all three processing steps can be carried forward into device fabrication.
  • Each cap material responds differently to annealing, resist removal, and acid cleaning, so the ranking is process-specific.
  • Resonator measurements serve as the final validation step for the layers that pass the XPS screen.
  • The non-destructive nature of XPS allows many candidate caps to be evaluated without committing to full device runs.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • The same XPS workflow could be applied to other oxidizable superconductors such as aluminum or tantalum films.
  • If XPS oxygen readings correlate tightly with measured loss tangents, early screening could replace some cryogenic tests during material development.
  • Room-temperature XPS results leave open the question of how the selected caps perform after cooldown and under prolonged operation.

Load-bearing premise

The oxidation and contamination levels seen at the surface by XPS correctly predict the dielectric losses that will appear once the same bilayers are made into complete superconducting resonators.

What would settle it

Building resonators from the XPS-downselected caps and measuring internal quality factors that show no improvement over uncapped niobium or that correlate poorly with the XPS oxygen signals.

Figures

Figures reproduced from arXiv: 2601.21953 by Maciej W. Olszewski, Tathagata Banerjee, Valla Fatemi.

Figure 1
Figure 1. Figure 1: FIG. 1. Schematic of X-rays entering the measured sample. [PITH_FULL_IMAGE:figures/full_fig_p001_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: FIG. 2. Nb 3d core level spectrum of (a) uncapped niobium [PITH_FULL_IMAGE:figures/full_fig_p002_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: FIG. 3. The relative oxidation of the Nb for the unprocessed [PITH_FULL_IMAGE:figures/full_fig_p003_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: FIG. 4. Results of acid cleaning of Nb-metal bilayers. 2% [PITH_FULL_IMAGE:figures/full_fig_p004_4.png] view at source ↗
Figure 5
Figure 5. Figure 5: FIG. 5. Resonator measurements a Nb resonator and capped [PITH_FULL_IMAGE:figures/full_fig_p005_5.png] view at source ↗
read the original abstract

Superconducting resonators and qubits are limited by dielectric losses from surface oxides. Surface oxides are mitigated through various strategies such as the addition of a metal capping layer, surface passivation, and acid processing. In this study, we demonstrate the use of X-ray photoelectron spectroscopy (XPS) as a rapid characterization tool to study the effectiveness cap layers for niobium for further device fabrication. We non-destructively evaluate 17 capping layers to characterize their ability to prevent oxygen diffusion, and the effects of standard fabrication processes -- annealing, resist stripping, and acid cleaning. We downselect for resilient capping layers and test their microwave resonator performance.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

2 major / 2 minor

Summary. The manuscript describes an experimental study using X-ray photoelectron spectroscopy (XPS) as a non-destructive tool to evaluate 17 capping layers on niobium surfaces. The authors characterize the layers' ability to block oxygen diffusion and their resilience to standard fabrication steps (annealing, resist stripping, acid cleaning), downselect promising candidates, and validate selected layers via microwave resonator measurements.

Significance. If the XPS metrics are shown to correlate quantitatively with reduced dielectric loss in completed devices, the work would offer a practical, rapid screening protocol for surface passivation strategies in superconducting quantum hardware, potentially shortening iteration cycles for low-loss resonators.

major comments (2)
  1. [Microwave resonator performance] Microwave resonator performance section: no quantitative correlation (e.g., oxygen at.% from XPS versus measured internal Q or tan δ) is reported for the down-selected capping layers. Without this link, the claim that XPS screening predicts device-level oxidation and loss cannot be evaluated.
  2. [Results] Results on fabrication-process effects: the manuscript does not present control data isolating whether additional lithography or etch steps (beyond the tested annealing/resist/acid sequence) reintroduce oxygen at the buried Nb interface, which is required to confirm that the XPS protocol on simplified bilayers captures the full fabrication flow.
minor comments (2)
  1. [Abstract] Abstract: quantitative results (oxygen percentages, Q values, or statistical significance of downselection) are absent, limiting the reader's ability to gauge the strength of the findings from the summary alone.
  2. [Methods and Figures] Figure captions and methods: error bars, number of replicates, and XPS quantification details (peak-fitting routines, sensitivity factors) are not specified, hindering reproducibility.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for their insightful comments, which have helped us improve the manuscript. We address the major comments below and have made revisions where appropriate to strengthen the connection between XPS metrics and device performance as well as to clarify the fabrication process coverage.

read point-by-point responses
  1. Referee: [Microwave resonator performance] Microwave resonator performance section: no quantitative correlation (e.g., oxygen at.% from XPS versus measured internal Q or tan δ) is reported for the down-selected capping layers. Without this link, the claim that XPS screening predicts device-level oxidation and loss cannot be evaluated.

    Authors: We agree that a direct quantitative correlation would better support our claims. The original manuscript presented resonator performance data for the down-selected layers but did not plot it against the XPS oxygen percentages. We have added this correlation analysis in the revised manuscript (new Figure 7), showing that lower oxygen at.% from XPS corresponds to higher internal Q factors, thereby validating the predictive capability of the XPS screening protocol. revision: yes

  2. Referee: [Results] Results on fabrication-process effects: the manuscript does not present control data isolating whether additional lithography or etch steps (beyond the tested annealing/resist/acid sequence) reintroduce oxygen at the buried Nb interface, which is required to confirm that the XPS protocol on simplified bilayers captures the full fabrication flow.

    Authors: The referee correctly notes the absence of such control data. Our experiments were focused on the sequence of annealing, resist stripping, and acid cleaning as these are the fabrication steps that directly follow capping layer deposition and are most relevant to oxidation at the Nb interface. We have revised the manuscript to include a discussion of this scope, noting that the XPS method is a rapid screening tool for these critical steps. Additional lithography and etch steps occur on the top surface and their effects are mitigated by the capping layer; however, we acknowledge that dedicated controls for the complete flow would provide further confirmation and have added this as a noted limitation in the revised Discussion section. revision: partial

Circularity Check

0 steps flagged

Purely experimental XPS characterization study with no derivations or self-referential predictions

full rationale

The manuscript is a materials characterization study that fabricates Nb/capping-layer test coupons, subjects them to standard fabrication steps (annealing, resist strip, acid clean), performs XPS surface analysis to quantify oxygen diffusion, down-selects resilient caps on the basis of those direct measurements, and then fabricates and measures microwave resonators on the selected caps. No equations, fitted models, or predictive relations are introduced; the down-selection criterion is the observed XPS oxygen signal itself, and the final resonator data serve as an independent experimental check rather than a quantity derived from the XPS results by construction. No self-citations are invoked to justify uniqueness or to close any logical loop. The entire chain is therefore self-contained experimental observation and comparison, with no reduction of any claimed result to its own inputs.

Axiom & Free-Parameter Ledger

0 free parameters · 0 axioms · 0 invented entities

Experimental materials study; no free parameters, axioms, or invented entities are identifiable from the abstract.

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Reference graph

Works this paper leans on

56 extracted references · 56 canonical work pages · 1 internal anchor

  1. [1]

    We detail the identical process here for completeness

    Resonator fabrication Resonators were fabricated as done in prior work [ 25]. We detail the identical process here for completeness. Wafers were prepared for deposition with an RCA clean, which is done by conducting SC-1 at 70 ◦C (1:1:6 ammo- nium hydroxide, hydrogen peroxide and water), SC-2 at 70 ◦C (1:1:6 hydrochloric acid, hydrogen peroxide and water)...

  2. [2]

    The fridge wiring diagram is shown in Figure S6

    F ridge setup The fridge used for the resonator measurements is a Bluefors small diameter refrigerator with a base tempera- ture of 500 mK. The fridge wiring diagram is shown in Figure S6. The input lines have about 10 dB of attenua- tion from the lines themselves and 60 dB attenuation from the attenuators. The output line has an dual junction isolator, a...

  3. [3]

    Measurement and analysis The resonator design has a 3µm gap between the cen- ter conductor and the ground plane and has a hangar resonator configuration, with eight λ/4 resonators at fre- 300 K 50 K 4 K 500 mK Amplifier Attenuator IR Filter Attenuator ProgrammableP Isolator IR HEMT 20 dB 20 dB 20 dB VNA IR IR Sample P 5-60 dB FIG. S6. Fridge wiring diagra...

  4. [4]

    Survey spectra are shown in Fig

    Resonator XPS To ensure consistency, one sample from each set of bilayers was measured in the XPS. Survey spectra are shown in Fig. S7 and the relative atomic percentage are given in Tab. S3. All resonators show comparable surface contamination similar to the previous measurements (Table I), however the control has the lowest carbon contamination. The Si ...

  5. [5]

    C. R. H. McRae, H. Wang, J. Gao, M. R. Vissers, T. Brecht, A. Dunsworth, D. P. Pappas, and J. Mutus, Review of Scientific Instruments91, 091101 (2020)

  6. [6]

    C. E. Murray, Materials Science and Engineering: R: Reports146, 100646 (2021)

  7. [7]

    M. Bal, A. A. Murthy, S. Zhu, F. Crisa, X. You, Z. Huang, T. Roy, J. Lee, D. V. Zanten, R. Pilipenko, I. Nekrashe- vich, A. Lunin, D. Bafia, Y. Krasnikova, C. J. Kopas, E. O. Lachman, D. Miller, J. Y. Mutus, M. J. Reagor, H. Cansizoglu, J. Marshall, D. P. Pappas, K. Vu, K. Ya- davalli, J.-S. Oh, L. Zhou, M. J. Kramer, F. Lecocq, D. P. Goronzy, C. G. Torre...

  8. [8]

    Tuokkola, Y

    M. Tuokkola, Y. Sunada, H. Kivij¨ arvi, J. Albanese, L. Gr¨ onberg, J.-P. Kaikkonen, V. Vesterinen, J. Gove- nius, and M. M¨ ott¨ onen, Nature Communications16, 5421 (2025)

  9. [9]

    M. P. Bland, F. Bahrami, J. G. C. Martinez, P. H. Preste- gaard, B. M. Smitham, A. Joshi, E. Hedrick, S. Kumar, A. Yang, A. C. Pakpour-Tabrizi, A. Jindal, R. D. Chang, G. Cheng, N. Yao, R. J. Cava, N. P. De Leon, and A. A. Houck, Nature 10.1038/s41586-025-09687-4 (2025)

  10. [10]

    R. D. Chang, N. Shumiya, R. A. McLellan, Y. Zhang, M. P. Bland, F. Bahrami, J. Mun, C. Zhou, K. Kisslinger, G. Cheng, B. M. Smitham, A. C. Pakpour-Tabrizi, N. Yao, Y. Zhu, M. Liu, R. J. Cava, S. Gopalakrishnan, A. A. Houck, and N. P. De Leon, Physical Review Letters134, 097001 (2025)

  11. [11]

    Burnett, L

    J. Burnett, L. Faoro, and T. Lindstr¨ om, Superconductor Science and Technology29, 044008 (2016)

  12. [12]

    N. P. de Leon, K. M. Itoh, D. Kim, K. K. Mehta, T. E. Northup, H. Paik, B. S. Palmer, N. Samarth, S. Sangtawesin, and D. W. Steuerman, Science372, eabb2823 (2021)

  13. [13]

    K. D. Crowley, R. A. McLellan, A. Dutta, N. Shumiya, A. P. Place, X. H. Le, Y. Gang, T. Madhavan, M. P. Bland, R. Chang, N. Khedkar, Y. C. Feng, E. A. Umbarkar, X. Gui, L. V. Rodgers, Y. Jia, M. M. Feldman, S. A. Lyon, M. Liu, R. J. Cava, A. A. Houck, and N. P. De Leon, Physical Review X13, 041005 (2023)

  14. [14]

    A. A. Murthy, M. Bal, M. J. Bedzyk, H. Cansizoglu, R. K. Chan, V. Chandrasekhar, F. Crisa, A. Datta, Y. Deng, C. D. M. Diaz, V. P. Dravid, D. A. Garcia- Wetten, S. Garattoni, S. Ghimire, D. P. Goronzy, S. d. Graaf, S. Haeuser, M. C. Hersam, D. Isheim, K. Joshi, R. Kim, S. Kolachina, C. J. Kopas, M. J. Kramer, E. O. Lachman, J. Lee, P. G. Lim, A. Lunin, W....

  15. [15]

    Y. V. Krasnikova, A. A. Murthy, D. Bafia, F. Crisa, A. Clairmont, Z. Sung, J. Lee, A. Cano, M. Shinde, D. M. T. v. Zanten, M. Bal, A. Romanenko, A. Grassellino, R. Dhundwal, D. Fuchs, T. Reisinger, I. M. Pop, A. Suter, T. Prokscha, and Z. Salman, Experimental Observation of Short-Range Magnetic Correlations in Amorphous Nb2O5 and Ta2O5 Thin Films (2025), ...

  16. [16]

    A. A. Murthy, P. Masih Das, S. M. Ribet, C. Kopas, J. Lee, M. J. Reagor, L. Zhou, M. J. Kramer, M. C. Hersam, M. Checchin, A. Grassellino, R. d. Reis, V. P. Dravid, and A. Romanenko, ACS Nano16, 17257 (2022)

  17. [17]

    Romanenko, R

    A. Romanenko, R. Pilipenko, S. Zorzetti, D. Frolov, M. Awida, S. Belomestnykh, S. Posen, and A. Grassellino, Physical Review Applied13, 034032 (2020)

  18. [18]

    Bafia, A

    D. Bafia, A. Murthy, A. Grassellino, and A. Romanenko, Physical Review Applied22, 024035 (2024)

  19. [19]

    Wenskat, J

    M. Wenskat, J. ˇCiˇ zek, M. O. Liedke, M. Butterling, M. Stiehl, G. D. L. Semione, C. Backes, C. Bate, O. Me- likhova, E. Hirschmann, A. Wagner, H. Weise, A. Stierle, M. Aeschlimann, and W. Hillert, Physical Review B106, 094516 (2022)

  20. [20]

    M. V. P. Alto´ e, A. Banerjee, C. Berk, A. Hajr, A. Schwartzberg, C. Song, M. Alghadeer, S. Aloni, M. J. Elowson, J. M. Kreikebaum, E. K. Wong, S. M. Griffin, S. Rao, A. Weber-Bargioni, A. M. Minor, D. I. Santiago, S. Cabrini, I. Siddiqi, and D. F. Ogletree, PRX Quantum 3, 020312 (2022)

  21. [21]

    M. C. De Ory, V. Rollano, D. Rodriguez, M. T. Magaz, D. Granados, and A. Gomez, Advanced Quantum Tech- nologies , 2400699 (2025)

  22. [22]

    C. Zhou, J. Mun, J. Yao, A. K. Anbalagan, M. D. Hossain, R. A. McLellan, R. Li, K. Kisslinger, G. Li, X. Tong, A. R. Head, C. Weiland, S. L. Hulbert, A. L. Walter, Q. Li, Y. Zhu, P. V. Sushko, and M. Liu, Advanced Materials 36, 2310280 (2024)

  23. [23]

    S. K. Karuppannan, D. Huang, N. M. Kommanaboina, K. Anil, G. Yan, D. V. M. Repaka, Y. Zhang, K. E. J. Goh, W. S. Kai, N. L. Chee Beng, Y. L. K. Sherry, and M. Mukherjee, ACS Applied Electronic Materials6, 7372 (2024)

  24. [24]

    Alghadeer, A

    M. Alghadeer, A. Banerjee, A. Hajr, H. Hussein, H. Fari- borzi, and S. G. Rao, ACS Applied Materials & Interfaces 15, 2319 (2023)

  25. [25]

    Zheng, D

    K. Zheng, D. Kowsari, N. J. Thobaben, X. Du, X. Song, S. Ran, E. A. Henriksen, D. S. Wisbey, and K. W. Murch, Applied Physics Letters120, 102601 (2022)

  26. [26]

    Verjauw, A

    J. Verjauw, A. Potoˇ cnik, M. Mongillo, R. Acharya, F. Mo- hiyaddin, G. Simion, A. Pacco, T. Ivanov, D. Wan, A. Van- leenhove, L. Souriau, J. Jussot, A. Thiam, J. Swerts, X. Piao, S. Couet, M. Heyns, B. Govoreanu, and I. Radu, Physical Review Applied16, 014018 (2021)

  27. [27]

    M. A. Gingras, B. M. Niedzielski, K. A. Grossklaus, D. Miller, F. Contipelli, K. Azar, L. D. Burkhart, G. Calu- sine, D. Davis, R. D. Pi˜ nero, J. M. Gertler, T. M. Hazard, C. F. Hirjibehedin, D. K. Kim, J. M. Knecht, A. J. Melville, C. O’Connell, R. A. Rood, A. Sab- bah, H. Stickler, J. L. Yoder, W. D. Oliver, M. E. Schwartz, and K. Serniak, Improving Tr...

  28. [28]

    C. J. Powell, Journal of Vacuum Science & Technology A: Vacuum, Surfaces, and Films38, 023209 (2020)

  29. [29]

    M. W. Olszewski, J. T. Paustian, T. Banerjee, H. Lu, J. L. Ramirez, N. Nguyen, K. Okubo, R. Pant, A. B. Biedron, D. C. Ralph, C. J. K. Richardson, G. D. Fuchs, C. R. H. 15 McRae, I. V. Pechenezhskiy, B. L. T. Plourde, and V. Fatemi, Low-loss Nb on Si superconducting resonators from a dual-use spintronics deposition chamber and with acid-free post-processi...

  30. [30]

    A. P. M. Place, L. V. H. Rodgers, P. Mundada, B. M. Smitham, M. Fitzpatrick, Z. Leng, A. Premkumar, J. Bryon, A. Vrajitoarea, S. Sussman, G. Cheng, T. Mad- havan, H. K. Babla, X. H. Le, Y. Gang, B. J¨ ack, A. Gyenis, N. Yao, R. J. Cava, N. P. De Leon, and A. A. Houck, Nature Communications12, 1779 (2021)

  31. [31]

    C. G. Torres-Castanedo, D. P. Goronzy, T. Pham, A. Mc- Fadden, N. Materise, P. Masih Das, M. Cheng, D. Lebe- dev, S. M. Ribet, M. J. Walker, D. A. Garcia-Wetten, C. J. Kopas, J. Marshall, E. Lachman, N. Zhelev, J. A. Sauls, J. Y. Mutus, C. R. H. McRae, V. P. Dravid, M. J. Bedzyk, and M. C. Hersam, Advanced Functional Mate- rials , 2401365 (2024)

  32. [32]

    C. J. Kopas, E. Lachman, C. R. H. McRae, Y. Mohan, J. Y. Mutus, A. Nersisyan, and A. Poudel, Simple copla- nar waveguide resonator mask targeting metal-substrate interface (2022), arXiv:2204.07202 [quant-ph]

  33. [33]

    M. S. Khalil, M. J. A. Stoutimore, F. C. Wellstood, and K. D. Osborn, Journal of Applied Physics111, 054510 (2012)

  34. [34]

    J. Choi, M. Olszewski, L. Zhang, Z. Baraissov, T. Baner- jee, K. Aggarwal, S. Chaudhari, T. A. Arias, D. A. Muller, V. Fatemi, and G. D. Fuchs, APL Materials13, 111103 (2025)

  35. [35]

    G. J. Dolan, Applied Physics Letters31, 337 (1977)

  36. [36]

    C. M. Quintana, A. Megrant, Z. Chen, A. Dunsworth, B. Chiaro, R. Barends, B. Campbell, Y. Chen, I.-C. Hoi, E. Jeffrey, J. Kelly, J. Y. Mutus, P. J. J. O’Malley, C. Neill, P. Roushan, D. Sank, A. Vainsencher, J. Wenner, T. C. White, A. N. Cleland, and J. M. Martinis, Applied Physics Letters105, 062601 (2014)

  37. [37]

    Muthusubramanian, M

    N. Muthusubramanian, M. Finkel, P. Duivestein, C. Zachariadis, S. L. M. Van Der Meer, H. M. Veen, M. W. Beekman, T. Stavenga, A. Bruno, and L. DiCarlo, Quantum Science and Technology9, 025006 (2024)

  38. [38]

    Logothetidis, E

    S. Logothetidis, E. Meletis, G. Stergioudis, and A. Ad- jaottor, Thin Solid Films338, 304 (1999)

  39. [39]

    A. V. Lubenchenko, A. B. Pavolotsky, S. Krause, O. I. Lubenchenko, D. A. Ivanov, V. Desmaris, and V. Belitsky, 30th International Symposium on Space THz Technology (2019)

  40. [40]

    M. Zier, S. Oswald, R. Reiche, and K. Wetzig, Applied Surface Science252, 234 (2005)

  41. [41]

    P. A. S. Carvalho and R. H. Miwa, Journal of Applied Physics114, 063705 (2013)

  42. [42]

    Dickey, Surface Science50, 515 (1975)

    J. Dickey, Surface Science50, 515 (1975)

  43. [43]

    Semione, A

    G. Semione, A. D. Pandey, S. Tober, J. Pfrommer, A. Poulain, J. Drnec, G. Sch¨ utz, T. Keller, H. Noei, V. Vonk, B. Foster, and A. Stierle, Physical Review Ac- celerators and Beams22, 103102 (2019)

  44. [44]

    Chaudhari, C

    S. Chaudhari, C. M´ endez, R. Choudhary, T. Banerjee, M. W. Olszewski, J. T. Paustian, J. Choi, Z. Baraissov, R. Hernandez, D. A. Muller, B. L. T. Plourde, G. D. Fuchs, V. Fatemi, and T. A. Arias, Active-Learning In- spired$ \textit{Ab Initio}$Theory-Experiment Loop Ap- proach for Management of Material Defects: Applica- tion to Superconducting Qubits (20...

  45. [45]

    AZ Electronic Materials, AZ 300T Stripper Safety Data Sheet (2015)

  46. [46]

    A. A. Murthy, J. Lee, C. Kopas, M. J. Reagor, A. P. McFadden, D. P. Pappas, M. Checchin, A. Grassellino, and A. Romanenko, Applied Physics Letters120, 044002 (2022)

  47. [47]

    Wenner, R

    J. Wenner, R. Barends, R. C. Bialczak, Y. Chen, J. Kelly, E. Lucero, M. Mariantoni, A. Megrant, P. J. J. O’Malley, D. Sank, A. Vainsencher, H. Wang, T. C. White, Y. Yin, J. Zhao, A. N. Cleland, and J. M. Martinis, Applied Physics Letters99, 113513 (2011)

  48. [48]

    Banerjee and V

    T. Banerjee and V. Fatemi, Dataset for ”Fabrication ef- fects on Niobium oxidation and surface contamination in Niobium-metal bilayers using X-ray photoelectron spec- troscopy” (2026)

  49. [49]

    Fairley, V

    N. Fairley, V. Fernandez, M. Richard-Plouet, C. Guillot- Deudon, J. Walton, E. Smith, D. Flahaut, M. Greiner, M. Biesinger, S. Tougaard, D. Morgan, and J. Baltrusaitis, Applied Surface Science Advances5, 100112 (2021)

  50. [50]

    Gorham, NIST X-ray Photoelectron Spectroscopy Database - SRD 20 (2012)

    J. Gorham, NIST X-ray Photoelectron Spectroscopy Database - SRD 20 (2012)

  51. [51]

    T. B. Reed,Free energy of formation of binary compounds: an atlas of charts for high-temperature chemical calcula- tions(MIT Press, Cambridge, Mass, 1971)

  52. [52]

    P. G. Baity, C. Maclean, V. Seferai, J. Bronstein, Y. Shu, T. Hemakumara, and M. Weides, Physical Review Re- search6, 013329 (2024)

  53. [53]

    Krinner, S

    S. Krinner, S. Storz, P. Kurpiers, P. Magnard, J. Heinsoo, R. Keller, J. Luetolf, C. Eichler, and A. Wallraff, EPJ Quantum Technology6, 2 (2019)

  54. [54]

    Fischer and G

    P. Fischer and G. Catelani, Physical Review Applied19, 054087 (2023)

  55. [55]

    Zmuidzinas, Annual Review of Condensed Matter Physics3, 169 (2012)

    J. Zmuidzinas, Annual Review of Condensed Matter Physics3, 169 (2012)

  56. [56]

    Gao,The Physics of Superconducting Microwave Res- onators, Ph.D

    J. Gao,The Physics of Superconducting Microwave Res- onators, Ph.D. thesis, California Institute of Technology, Pasadena, California (2008)