Cited by 198High Entropy Alloys StudiesPhysics of Superconductivity and MagnetismSuperconducting Materials and Applications

Effect of electron count and chemical complexity in the Ta-Nb-Hf-Zr-Ti high-entropy alloy superconductor

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von Rohr, Fabian, Winiarski, Michał J., Tao, Jing, Klimczuk, Tomasz, Cava, Robert Joseph·2016·Proceedings of the National Academy of Sciences

Abstract

Significance: High-entropy alloys are a new class of materials that consist of several principal elements arranged on simple lattices. These structures are stabilized by the high configurational entropy of the random mixing of the elements. Here, we show that the properties of a superconducting high-entropy alloy are strongly related to the electron count and that the superconducting transition temperatures of these alloys fall between those of analogous crystalline and amorphous materials. We find that despite the large degree of randomness and disorder in these alloys, the superconducting properties are nevertheless strongly dependent on the chemical composition and complexity. We argue that high-entropy alloys are excellent model systems for understanding how superconductivity and other collective quantum states evolve from crystals to amorphous solids.

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Crossref · 10.1073/pnas.1615926113

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  • The Ta-Hf-Nb-Zr-Ti system has emerged as the most extensively investigated BCC-type HEA superconductor.

    “The Ta-Hf-Nb-Zr-Ti system has emerged as the most extensively investigated BCC-type HEA superconductor 9 -17 .”

    From Recent advances in high-entropy superconductors (2024) · cites this paper as [9]

    The introduction (p. 2) identifies Ta-Nb-Hf-Zr-Ti as a BCC high-entropy-alloy superconductor, and the Summary and Conclusion (p. 7) report investigations of multiple compositions. The paper does not compare how extensively this system has been investigated with other BCC HEA superconductors, so it does not establish “most extensively investigated.” (LLM, conf=0.86)

    Experimental — accuracy not yet measured
  • The atomic disorder present in the BCC-type HEAs has a minimal influence on the superconducting state, as Tc is insensitive to disorder in both simple crystalline and amorphous metallic states.

    “Thus, the atomic disorder present in the BCC-type HEAs has a minimal in fl uence on the superconducting state, as T c is insensitive to disorder in both simple crystalline and amorphous metallic states.”

    From Recent advances in high-entropy superconductors (2024) · cites this paper as [9]

    The Significance section (p. 5) reports that increasing atomic disorder from a binary alloy to the BCC HEA causes very little decrease in Tc, supporting the claim about the HEA. The paper compares Tc trends in crystalline alloys and amorphous films (p. 4), but does not say Tc is insensitive to disorder in both of those states. (LLM, conf=0.83)

    Experimental — accuracy not yet measured
  • The Tc range is approximately 2-8 K in BCC-type HEA superconductors.

    “The T c range is approximately 2 -8 K in BCC-type HEA superconductors.”

    From Recent advances in high-entropy superconductors (2024) · cites this paper as [9]

    The Summary and Conclusion (p. 7) says all studied Ta-Nb-Hf-Zr-Ti HEAs have a BCC lattice and reports superconducting critical temperatures of approximately 4.49–7.92 K. This supports the upper end of the claimed range, but the paper does not establish a lower bound near 2 K or that the range applies to BCC-type HEA superconductors generally. (LLM, conf=0.88)

    Experimental — accuracy not yet measured
  • Experimental evidence has indicated that the VEC of HEA and HEC superconductors is critical in determining their superconducting Tc and material stability.

    “Experimental evidence has indicated that the VEC of HEA and HEC superconductors is critical in determining their superconducting T c and material stability.”

    From Recent advances in high-entropy superconductors (2024) · cites this paper as [9]

    The Summary and Conclusion (p. 7) reports a dependence of superconducting Tc on valence electron count in the Ta-Nb-Hf-Zr-Ti HEA. But the Significance section (p. 3) says high entropy stabilizes its BCC structure even where electron count would predict HCP, so the paper does not establish VEC as critical to this material’s stability. It also does not study HEC superconductors. (LLM, conf=0.87)

    Experimental — accuracy not yet measured
  • The upper critical fields appear to increase with increasing entropy in some high-entropy systems.

    “Furthermore, the upper critical fi elds appear to increase with increasing entropy in some high-entropy systems 9,44,70 .”

    From Recent advances in high-entropy superconductors (2024) · cites this paper as [9]

    The upper-critical-fields discussion (p. 5) says the slopes of the upper critical fields increase with mixing entropy. It does not establish the same trend for the upper critical field values: the x = 0.5 sample has the largest field, while x = 0.84 has the greatest mixing entropy. (LLM, conf=0.86)

    Experimental — accuracy not yet measured

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Cites

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Research works printed but not linked: 3

  1. [26]Orlando TP, McNiff EJ, Jr, Foner S, Beasley MR (1979) Critical fields, Pauli paramagnetic limiting, and material parameters of Nb3Sn and V3Si. Phys Rev B 19(9):4545.
  2. [29]Werthamer NR, Helfand E, Hohenberg PC (1966) Temperature and purity dependence of the superconducting critical field. Phys Rev 147(1):295.
  3. [39]Hirai D, von Rohr F, Cava RJ (2012) Emergence of superconductivity in BaNi2 ð Ge1 -x P x Þ 2 at a structural instability. Phys Rev B 86(10):100505(R).

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Authors
von Rohr, F., Winiarski, M. J., Tao, J., Klimczuk, T., & Cava, R. J.
Affiliations
  • Department of Chemistry, Princeton University, Princeton, NJ 08544;
  • Faculty of Applied Physics and Mathematics, Gdansk University of Technology, Gdansk 80-233, Poland;
  • Brookhaven National Laboratory (US)
  • Gdańsk University of Technology (PL)
  • Princeton University (US)
Venue
Proceedings of the National Academy of Sciences
Published
2016-11
Volume
113
Issue
46
Pages
E7144-E7150
ISSN
  • 0027-8424 (ISSN-L)
  • 1091-6490
OpenAlex
W2535364585
Cited by
198
References
39
Citations by year
2026: 15 · 2025: 30 · 2024: 36 · 2023: 25 · 2022: 24 · 2021: 23 · 2020: 19 · 2019: 11 · 2018: 12 · 2017: 3
FWCI
7.71
Type
journal article
Language
en
Open access
Locations
  • Proceedings of the National Academy of Sciences (publishedVersion)
  • PubMed Central (publishedVersion)
  • PubMed (publishedVersion)
  • Archive ouverte UNIGE (University of Geneva) (publishedVersion, other-oa)
  • arXiv (Cornell University) (submittedVersion)
  • OSTI OAI (U.S. Department of Energy Office of Scientific and Technical Information) (submittedVersion)
  • Archive ouverte UNIGE (University of Geneva) (submittedVersion, cc-by)
  • arXiv (Cornell University)
Funders
  • Gordon and Betty Moore Foundation (Grant GBMF-4412)
  • Narodowe Centrum Nauki (DEC-2012/07/E/ST3/00584)
  • DOE | Brookhaven National Laboratory, Office of Science (DE-AC02-98CH10886)
Topics
  • Physical Sciences › Engineering › Mechanical Engineering › High Entropy Alloys Studies
  • Physical Sciences › Physics and Astronomy › Condensed Matter Physics › Physics of Superconductivity and Magnetism
  • Physical Sciences › Engineering › Biomedical Engineering › Superconducting Materials and Applications
Keywords
high-entropy alloys, superconductivity, valence electron count, superconducting transition temperature, body-centered cubic lattice, amorphous materials, disorder robustness, solid solutions

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