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Violation of Matthias rule: Elemental composition as the key determinant of critical temperature in bcc high-entropy superconductors

Rafał Idczak1,*, Wojciech Nowak1,2, Michał Babij2, Daniel Gnida2, Robert Konieczny1, Monika K. Krawczyk1, Dorota Podsiadła1, Tomasz Ossowski1, Rafał Topolnicki1,3 et al.

Adam Pikul2

  • *Contact author: rafal.idczak@uwr.edu.pl

Phys. Rev. B 112, 014513 – Published 16 July, 2025

DOI: https://doi.org/10.1103/fnz7-bzmw

Abstract

We systematically investigate three body-centred cubic (bcc) high-entropy alloys (HEAs) with an identical valence electron count (VEC = 4.375): (NbHf)0.75(TiZr)0.25, (NbZr)0.75(TiHf)0.25, and (NbTi)0.75(ZrHf)0.25. Despite their isoelectronic nature, it was found that these alloys exhibit markedly different superconducting properties. Critical temperatures Tc range from 7.14(5) K to 8.17(5) K, while upper critical fields μ0Hc2(0) exceed 12 T, reaching 14.0(9) T for the Ti-rich alloy (NbTi)0.75(ZrHf)0.25. These variations highlight the limited predictive power of the Matthias rule in HEA design. Furthermore, the exceptional properties observed in the Ti-rich composition suggest that Nb and Ti are critical elements for the development of new HEAs for next-generation superconducting magnets.

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References (48)

  1. J.-W. Yeh, S.-K. Chen, S.-J. Lin, J.-Y. Gan, T.-S. Chin, T.-T. Shun, C.-H. Tsau, and S.-Y. Chang, Nanostructured high-entropy alloys with multiple principal elements: Novel alloy design concepts and outcomes, Adv. Eng. Mater. 6, 299 (2004).
  2. B. Cantor, I. Chang, P. Knight, and A. Vincent, Microstructural development in equiatomic multicomponent alloys, Mater. Sci. Eng.: A 375-377, 213 (2004).
  3. P. Koželj, S. Vrtnik, A. Jelen, S. Jazbec, Z. Jagličić, S. Maiti, M. Feuerbacher, W. Steurer, and J. Dolinšek, Discovery of a superconducting high-entropy alloy, Phys. Rev. Lett. 113, 107001 (2014).
  4. L. Sun and R. J. Cava, High-entropy alloy superconductors: Status, opportunities, and challenges, Phys. Rev. Mater. 3, 090301 (2019).
  5. L. Zeng, L. Li, K. Li, R. Chen, and H. Luo, Recent advances in high-entropy superconductors, NPG Asia Mater. 16, 60 (2024).
  6. J. Kitagawa, Y. Mizuguchi, and T. Nishizaki, High critical current densities of body-centered cubic high-entropy alloy superconductors: Recent research progress, Eur. Phys. J. B 98, 73 (2025).
  7. B. T. Matthias, Empirical relation between superconductivity and the number of valence electrons per atom, Phys. Rev. 97, 74 (1955).
  8. F. von Rohr, M. J. Winiarski, J. Tao, T. Klimczuk, and R. J. Cava, Effect of electron count and chemical complexity in the Ta-Nb-Hf-Zr-Ti high-entropy alloy superconductor, Proc. Natl. Acad. Sci. USA 113, E7144 (2016).
  9. L. Zeng, J. Zhan, M. Boubeche, K. Li, L. Li, P. Yu, K. Wang, C. Zhang, K. Jin, Y. Sun, and H. Luo, Superconductivity in the bcc-type high-entropy alloy TiHfNbTaMo, Adv. Quantum Technol. 6, 2300213 (2023).
  10. F. O. von Rohr and R. J. Cava, Isoelectronic substitutions and aluminium alloying in the Ta-Nb-Hf-Zr-Ti high-entropy alloy superconductor, Phys. Rev. Mater. 2, 034801 (2018).
  11. J. Rodríguez-Carvajals, Recent advances in magnetic structure determination by neutron powder diffraction, Phys. B: Condens. Matter 192, 55 (1993).
  12. P. Soven, Coherent-potential model of substitutional disordered alloys, Phys. Rev. 156, 809 (1967).
  13. G. D. Gaspari and B. L. Gyorffy, Electron-phonon interactions, d resonances, and superconductivity in transition metals, Phys. Rev. Lett. 28, 801 (1972).
  14. W. H. Butler, Theory of electronic transport in random alloys: Korringa-Kohn-Rostoker coherent-potential approximation, Phys. Rev. B 31, 3260 (1985).
  15. S. Kaprzyk and A. Bansil, Green's function and a generalized Lloyd formula for the density of states in disordered muffin-tin alloys, Phys. Rev. B 42, 7358 (1990).
  16. A. Bansil and S. Kaprzyk, First-principles treatment of disorder effects in complex alloys: A study of BaxK1−xBiO3 and BaPb1−xBixO3, Phys. Rev. B 43, 10335 (1991).
  17. H. Akai, Electronic structure Ni–Pd alloys calculated by the self-consistent KKR-CPA method, J. Phys. Soc. Jpn. 51, 468 (1982).
  18. H. Akai, Fast Korringa-Kohn-Rostoker coherent potential approximation and its application to FCC Ni-Fe systems, J. Phys.: Condens. Matter 1, 8045 (1989).
  19. T. Kotani and H. Akai, KKR-ASA method in exact exchange-potential band-structure calculations, Phys. Rev. B 54, 16502 (1996).
  20. J. P. Perdew and W. Yue, Accurate and simple density functional for the electronic exchange energy: Generalized gradient approximation, Phys. Rev. B 33, 8800 (1986).
  21. J. P. Perdew, K. Burke, and M. Ernzerhof, Generalized gradient approximation made simple, Phys. Rev. Lett. 77, 3865 (1996).
  22. J. P. Perdew, K. Burke, and Y. Wang, Generalized gradient approximation for the exchange-correlation hole of a many-electron system, Phys. Rev. B 54, 16533 (1996).
  23. F. Birch, Finite elastic strain of cubic crystals, Phys. Rev. 71, 809 (1947).
  24. G. Kresse and J. Hafner, Ab initio molecular dynamics for open-shell transition metals, Phys. Rev. B 48, 13115 (1993).
  25. G. Kresse and J. Furthmüller, Efficient iterative schemes for ab initio total-energy calculations using a plane-wave basis set, Phys. Rev. B 54, 11169 (1996).
  26. G. Kresse and J. Furthmüller, Efficiency of ab initio total energy calculations for metals and semiconductors using a plane-wave basis set, Comput. Mater. Sci. 6, 15 (1996).
  27. G. Kresse and D. Joubert, From ultrasoft pseudopotentials to the projector augmented-wave method, Phys. Rev. B 59, 1758 (1999).
  28. P. E. Blöchl, Projector augmented-wave method, Phys. Rev. B 50, 17953 (1994).
  29. O. N. Senkov, J. M. Scott, S. V. Senkova, D. B. Miracle, and C. F. Woodward, Microstructure and room temperature properties of a high-entropy TaNbHfZrTi alloy, J. Alloys Compd. 509, 6043 (2011).
  30. G. Williamson and W. Hall, X-ray line broadening from filed aluminium and wolfram, Acta Metall. 1, 22 (1953).
  31. A. Tari, The Specific Heat of Matter at Low Temperatures (World Scienfitic, Singapore, 2003).
  32. J. Bardeen, L. N. Cooper, and J. R. Schrieffer, Theory of superconductivity, Phys. Rev. 108, 1175 (1957).
  33. W. L. McMillan, Transition temperature of strong-coupled superconductors, Phys. Rev. 167, 331 (1968).
  34. P. B. Allen and R. C. Dynes, Transition temperature of strong-coupled superconductors reanalyzed, Phys. Rev. B 12, 905 (1975).
  35. E. Helfand and N. R. Werthamer, Temperature and purity dependence of the superconducting critical field, Hc2. II, Phys. Rev. 147, 288 (1966).
  36. N. R. Werthamer, E. Helfand, and P. C. Hohenberg, Temperature and purity dependence of the superconducting critical field, Hc2. III. electron spin and spin-orbit effects, Phys. Rev. 147, 295 (1966).
  37. K. Maki, Effect of Pauli paramagnetism on magnetic properties of high-field superconductors, Phys. Rev. 148, 362 (1966).
  38. A. M. Clogston, Upper limit for the critical field in hard superconductors, Phys. Rev. Lett. 9, 266 (1962).
  39. Y. Shapira and L. J. Neuringer, Upper critical fields of Nb-Ti alloys: Evidence for the influence of Pauli paramagnetism, Phys. Rev. 140, A1638 (1965).
  40. J. Kitagawa and Y. Mizuguchi, High-Entropy Alloy Superconductors: Exotic Properties, Applications and Materials Design, Springer Series in Solid-State Sciences (Springer Nature, Singapore, 2024).
  41. P. Sobota, B. Rusin, D. Gnida, R. Topolnicki, T. Ossowski, W. Nowak, A. Pikul, and R. Idczak, New type of Ti-rich HEA superconductors with high upper critical field, Acta Mater. 285, 120666 (2025).
  42. M. Krnel, A. Jelen, S. Vrtnik, J. Luzar, D. Gačnik, P. Koželj, M. Wencka, A. Meden, Q. Hu, S. Guo, and J. Dolinšek, The effect of scandium on the structure, microstructure and superconductivity of equimolar Sc-Hf-Nb-Ta-Ti-Zr refractory high-entropy alloys, Materials 15, 1122 (2022).
  43. R. D. Parks, Superconductivity: In Two Volumes: Volume 1 (Taylor & Francis, New York, 2019).
  44. M. Tinkham, Introduction to Superconductivity, International series in pure and applied physics (McGraw-Hill, New York, 1975).
  45. P. Sobota, R. Topolnicki, T. Ossowski, T. Pikula, A. Pikul, and R. Idczak, Superconductivity in the high-entropy alloy (NbTa)0.67(MoHfW)0.33, Phys. Rev. B 106, 184512 (2022).
  46. R. Idczak, W. Nowak, B. Rusin, R. Topolnicki, T. Ossowski, M. Babij, and A. Pikul, Enhanced superconducting critical parameters in a new high-entropy alloy Nb0.34Ti0.33Zr0.14Ta0.11Hf0.08, Materials 16, 5814 (2023).
  47. C. Kittel, Introduction to Solid State Physics, 7th ed. (Wiley, New York, 2007).
  48. OSF repository at https://osf.io/g4n6b/.

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