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First-principles evidence for conventional superconductivity in a quasicrystal approximant

Pedro N. Ferreira1,*, Roman Lucrezi2, Sangmin Lee3, Lucy Nathwani3, Matthew Julian4, Rohit P. Prasankumar4, Warren E. Pickett5, Chris J. Pickard6,7, Philip Kim3 et al.

Christoph Heil1,†

  • *Contact author: nunesferreira@tugraz.at
  • †Contact author: christoph.heil@tugraz.at

Phys. Rev. B 114, 074512 – Published 27 August, 2026

DOI: https://doi.org/10.1103/qx58-z229

Abstract

Quasicrystals (QCs) host long-range order without translational symmetry, a regime in which the very foundations of BCS theory are not straightforwardly applicable, yet experiments on QCs and their approximant crystals (ACs) point to conventional, s-wave, electron–phonon-coupled superconductivity. Here, we test the predictive power of the electron–phonon framework in a representative decagonal AC from first principles. Using state-of-the-art ab initio methods, we compute the superconducting properties of the recently discovered AC Al13Os4 and quantitatively reproduce its bulk Tc. This provides an ab initio determination of Tc for an AC and establishes that the electron–phonon framework is predictive in these systems. Using the generalized quasichemical approximation for alloy modeling in the decagonal Al–Os family, we predict tunable superconductivity in Al13Os4−xRex and Al13Os4−xIrx; in particular, Al13Re4 is dynamically stable and estimated to have a Tc about 30% above that of Al13Os4. Finally, we discuss the role of ACs as high-fidelity proxies for their parent QCs. Although long-range quasiperiodicity may introduce subtle electronic features, our findings indicate that the key ingredients for superconductivity are already encoded in the local structural motifs preserved by the AC. This places the Al–Os and Al–Re families among the most promising candidates for the highest-Tc quasicrystalline superconductivity.

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References (98)

  1. D. Levine and P. J. Steinhardt, Quasicrystals: A new class of ordered structures, Phys. Rev. Lett. 53, 2477 (1984).
  2. D. Levine and P. J. Steinhardt, Quasicrystals. I. Definition and structure, Phys. Rev. B 34, 596 (1986).
  3. J. E. S. Socolar and P. J. Steinhardt, Quasicrystals. II. Unit-cell configurations, Phys. Rev. B 34, 617 (1986).
  4. D. Shechtman, I. Blech, D. Gratias, and J. W. Cahn, Metallic phase with long-range orientational order and no translational symmetry, Phys. Rev. Lett. 53, 1951 (1984).
  5. W. Man, M. Megens, P. J. Steinhardt, and P. M. Chaikin, Experimental measurement of the photonic properties of icosahedral quasicrystals, Nature (London) 436, 993 (2005).
  6. M. C. Rechtsman, H.-C. Jeong, P. M. Chaikin, S. Torquato, and P. J. Steinhardt, Optimized structures for photonic quasicrystals, Phys. Rev. Lett. 101, 073902 (2008).
  7. M. Florescu, S. Torquato, and P. J. Steinhardt, Complete band gaps in two-dimensional photonic quasicrystals, Phys. Rev. B 80, 155112 (2009).
  8. C. Lin, P. J. Steinhardt, and S. Torquato, Light localization in local isomorphism classes of quasicrystals, Phys. Rev. Lett. 120, 247401 (2018).
  9. M. Yoshimura and A. Tsai, Quasicrystal application on catalyst, J. Alloys Compd. 342, 451 (2002).
  10. S. Kameoka, T. Tanabe, and A. P. Tsai, Al–Cu–Fe quasicrystals for steam reforming of methanol: A new form of copper catalysts, Catal. Today 93-95, 23 (2004).
  11. J. Dubois, S. Kang, P. Archambault, and B. Colleret, Thermal diffusivity of quasicrystalline and related crystalline alloys, J. Mater. Res. 8, 38 (1993).
  12. J.-M. Dubois, Properties-and applications of quasicrystals and complex metallic alloys, Chem. Soc. Rev. 41, 6760 (2012).
  13. A. I. Goldman, Magnetism in icosahedral quasicrystals: Current status and open questions, Sci. Technol. Adv. Mater. 15, 044801 (2014).
  14. R. Chen, C.-Z. Chen, J.-H. Gao, B. Zhou, and D.-H. Xu, Higher-order topological insulators in quasicrystals, Phys. Rev. Lett. 124, 036803 (2020).
  15. D. V. Else, S.-J. Huang, A. Prem, and A. Gromov, Quantum many-body topology of quasicrystals, Phys. Rev. X 11, 041051 (2021).
  16. T. Ishimasa, Y. Tanaka, and S. K. and, Icosahedral quasicrystal and 1/1 cubic approximant in Au–Al–Yb alloys, Philos. Mag. 91, 4218 (2011).
  17. T. Watanuki, S. Kashimoto, D. Kawana, T. Yamazaki, A. Machida, Y. Tanaka, and T. J. Sato, Intermediate-valence icosahedral Au–Al–Yb quasicrystal, Phys. Rev. B 86, 094201 (2012).
  18. K. Deguchi, S. Matsukawa, N. K. Sato, T. Hattori, K. Ishida, H. Takakura, and T. Ishimasa, Quantum critical state in a magnetic quasicrystal, Nat. Mater. 11, 1013 (2012).
  19. L. Bindi, V. E. Dmitrienko, and P. J. Steinhardt, Are quasicrystals really so rare in the universe? Am. Mineral. 105, 1121 (2020).
  20. J. E. Graebner and H. S. Chen, Specific heat of an icosahedral superconductor, Mg3Zn3Al2, Phys. Rev. Lett. 58, 1945 (1987).
  21. Although this phase might, in fact, be better classified as an approximant quasicrystal (AC) [98], which are periodic phases resulting from QC projections along rational directions.
  22. J. L. Wagner, B. D. Biggs, K. M. Wong, and S. J. Poon, Specific-heat and transport properties of alloys exhibiting quasicrystalline and crystalline order, Phys. Rev. B 38, 7436 (1988).
  23. V. Azhazha, A. Grib, G. Khadzhay, S. Malikhin, B. Merisov, and A. Pugachov, Superconductivity of Ti–Zr–Ni alloys containing quasicrystals, Phys. Lett. A 303, 87 (2002).
  24. K. Kamiya, T. Takeuchi, N. Kabeya, N. Wada, T. Ishimasa, A. Ochiai, K. Deguchi, K. Imura, and N. Sato, Discovery of superconductivity in quasicrystal, Nat. Commun. 9, 154 (2018).
  25. S. Sakai, N. Takemori, A. Koga, and R. Arita, Superconductivity on a quasiperiodic lattice: Extended-to-localized crossover of Cooper pairs, Phys. Rev. B 95, 024509 (2017).
  26. Y. Tokumoto, K. Hamano, S. Nakagawa, Y. Kamimura, S. Suzuki, R. Tamura, and K. Edagawa, Superconductivity in a van der Waals layered quasicrystal, Nat. Commun. 15, 1529 (2024).
  27. T. Terashima, Y. Tokumoto, K. Hamano, T. Konoike, N. Kikugawa, and K. Edagawa, Anomalous upper critical field in the quasicrystal superconductor Ta1.6Te, npj Quantum Mater. 9, 56 (2024).
  28. R. N. Araújo and E. C. Andrade, Conventional superconductivity in quasicrystals, Phys. Rev. B 100, 014510 (2019).
  29. B. Yavas, C. J. Hung, S. K. Nayak, M. Aindow, and S. P. Alpay, Quasicrystal stability in complex aluminum alloys: Insights from first principles models on structural motifs in crystalline approximants, Scr. Mater. 222, 115046 (2023).
  30. J. D. Cain, A. Azizi, M. Conrad, S. M. Griffin, and A. Zettl, Layer-dependent topological phase in a two-dimensional quasicrystal and approximant, Proc. Natl. Acad. Sci. USA 117, 26135 (2020).
  31. T. T. Dorini, F. Brix, C. Chatelier, A. Kokalj, and E. Gaudry, Two-dimensional oxide quasicrystal approximants with tunable electronic and magnetic properties, Nanoscale 13, 10771 (2021).
  32. P. K. Meena, R. Verma, Arushi, S. Jangid, R. K. Kushwaha, R. Stewart, A. D. Hillier, B. Singh, and R. P. Singh, Observation of superconductivity in a nontrivial Z2 approximant quasicrystal, Commun. Mater. 6, 226 (2025).
  33. L.-E. Edshammar, A. Stig, R. Torbjorn, and D. R. Sparrow, The crystal structure of Os4Al13, Acta Chem. Scand. 18, 2294 (1964).
  34. J.-N. Barbier, N. Tamura, and J.-L. Verger-Gaugry, Monoclinic Al13Fe4 approximant phase: A link between icosahedral and decagonal phases, J. Non-Cryst. Solids 153-154, 126 (1993).
  35. J. Grin, U. Burkhardt, M. Ellner, and K. Peters, Refinement of the Fe4Al13 structure and its relationship to the quasihomological homeotypical structures, Z. Kristallogr. Cryst. Mater. 209, 479 (1994).
  36. B. Zhang, V. Gramlich, and W. Steurer, Al13−x(Co1−yNiy)4, a new approximant of the decagonal quasicrystal in the Al–Co–Ni system, Z. Kristallogr. Cryst. Mater. 210, 498 (1995).
  37. K. Kuo, Some new icosahedral and decagonal quasicrystals, in Quasicrystals, Materials Science Forum, Vol. 22 (Trans Tech Publications Ltd., 1987), pp. 131–140.
  38. Z.-M. Wang, Y.-Q. Gao, and K. H. Kuo, Quasicrystals of rapidly solidified alloys of Al-Pt group metals: II. Quasicrystals in rapidly solidified Al-Ru and Al-Os alloys, J. Less-Common Met. 163, 19 (1990).
  39. W. Steurer, T. Haibach, B. Zhang, S. Kek, and R. Lück, The structure of decagonal Al70Ni15Co15, Acta Crystallogr. Sect. B: Struct. Sci. 49, 661 (1993).
  40. K. Berland, V. R. Cooper, K. Lee, E. Schröder, T. Thonhauser, P. Hyldgaard, and B. I. Lundqvist, Van der Waals forces in density functional theory: A review of the vdW-DF method, Rep. Prog. Phys. 78, 066501 (2015).
  41. D. Chakraborty, K. Berland, and T. Thonhauser, Next-generation nonlocal van der Waals density functional, J. Chem. Theory Comput. 16, 5893 (2020).
  42. A. D. Becke and K. E. Edgecombe, A simple measure of electron localization in atomic and molecular systems, J. Chem. Phys. 92, 5397 (1990).
  43. L. De Santis and R. Resta, Electron localization at metal surfaces, Surf. Sci. 450, 126 (2000).
  44. See Supplemental Material at http://link.aps.org/supplemental/10.1103/qx58-z229 for spin–orbit-coupling effects in Al13Os4, alloy thermodynamics, and electronic and phonon properties of Al13Ir4.
  45. M. Zehetmayer, A review of two-band superconductivity: Materials and effects on the thermodynamic and reversible mixed-state properties, Supercond. Sci. Technol. 26, 043001 (2013).
  46. A. Gurevich, Enhancement of the upper critical field by nonmagnetic impurities in dirty two-gap superconductors, Phys. Rev. B 67, 184515 (2003).
  47. A. Floris, A. Sanna, S. Massidda, and E. K. U. Gross, Two-band superconductivity in Pb from ab initio calculations, Phys. Rev. B 75, 054508 (2007).
  48. Y. Zhao, C. Lian, S. Zeng, Z. Dai, S. Meng, and J. Ni, MgB4 trilayer film: A four-gap superconductor, Phys. Rev. B 101, 104507 (2020).
  49. L. E. Correa, P. P. Ferreira, L. R. de Faria, T. T. Dorini, M. S. da Luz, Z. Fisk, M. S. Torikachvili, L. T. Eleno, and A. J. Machado, Evidence for multiband superconductivity and charge density waves in Ni-doped ZrTe2, J. Alloys Compd. 907, 164477 (2022).
  50. L. E. Correa, P. P. Ferreira, L. R. de Faria, V. M. Fim, M. S. da Luz, M. S. Torikachvili, C. Heil, L. T. F. Eleno, and A. J. S. Machado, Superconductivity in Te-deficient ZrTe2, J. Phys. Chem. C 127, 5162 (2023).
  51. H. Suhl, B. T. Matthias, and L. R. Walker, Bardeen-Cooper-Schrieffer theory of superconductivity in the case of overlapping bands, Phys. Rev. Lett. 3, 552 (1959).
  52. E. J. Nicol and J. P. Carbotte, Properties of the superconducting state in a two-band model, Phys. Rev. B 71, 054501 (2005).
  53. A. Y. Liu, I. I. Mazin, and J. Kortus, Beyond Eliashberg superconductivity in MgB2: Anharmonicity, two-phonon scattering, and multiple gaps, Phys. Rev. Lett. 87, 087005 (2001).
  54. I. I. Mazin, O. K. Andersen, O. Jepsen, O. V. Dolgov, J. Kortus, A. A. Golubov, A. B. Kuz'menko, and D. van der Marel, Superconductivity in MgB2: Clean or dirty? Phys. Rev. Lett. 89, 107002 (2002).
  55. G. Lamura, D. Tay, R. Khasanov, P. Gentile, C. Xu, X. Ke, I. Onuorah, P. Bonfà, X. Xu, and T. Shiroka, Anisotropic superconductivity in the quasi-one-dimensional superconductor V2Ga5, Sci. Rep. 15, 14185 (2025).
  56. T. Shang, D. Tay, H. Su, H. Q. Yuan, and T. Shiroka, Evidence of fully gapped superconductivity in NbReSi: A combined μSR and NMR study, Phys. Rev. B 105, 144506 (2022).
  57. T. Shiroka, T. Shang, M. Juckel, M. Krnel, M. König, U. Burkhardt, P. Koželj, R. Gupta, Y. Prots, and E. Svanidze, Superconductivity of MoBe22 and WBe22 at ambient- and under applied-pressure conditions, Phys. Rev. Materials 6, 064804 (2022).
  58. T. Shang, J. Meng, X. Y. Zhu, H. Zhang, B. C. Yu, Z. X. Zhen, Y. H. Wang, Y. Xu, Q. F. Zhan, D. J. Gawryluk, and T. Shiroka, Fully gapped superconductivity with preserved time-reversal symmetry in NiBi3 single crystals, Phys. Rev. B 107, 174513 (2023).
  59. T. Shang, E. Svanidze, and T. Shiroka, Probing the superconducting pairing of the La4Be33Pt16 alloy via muon-spin spectroscopy, J. Phys.: Condens. Matter 36, 105601 (2024).
  60. K. Panda, A. Bhattacharyya, P. N. Ferreira, R. Mondal, A. Thamizhavel, D. T. Adroja, C. Heil, L. T. F. Eleno, and A. D. Hillier, Probing the superconducting gap structure of ScRuSi via μSR and first-principles calculations, Phys. Rev. B 109, 224517 (2024).
  61. J. Kačmarčík, Z. Pribulová, T. Shiroka, F. Kosuth, P. Szabó, M. Winiarski, S. Królak, J. Jaroszynski, T. Shang, R. Cava, C. Marcenat, T. Klein, T. Klimczuk, and P. Samuely, Single-gap two-band superconductivity well above the Pauli limit in non-centrosymmetric TaIr2B2, Superconductivity 14, 100167 (2025).
  62. T. Shang, J. Zhao, K. Xia, L.-H. Hu, Y. Xu, Q. Zhan, D. J. Gawryluk, and T. Shiroka, Multiband superconductivity in the topological Kramers nodal-line semimetals, Phys. Rev. B 111, 214516 (2025).
  63. E. R. Margine and F. Giustino, Anisotropic Migdal-Eliashberg theory using Wannier functions, Phys. Rev. B 87, 024505 (2013).
  64. R. Lucrezi, P. P. Ferreira, S. Hajinazar, H. Mori, H. Paudyal, E. R. Margine, and C. Heil, Full-bandwidth anisotropic Migdal-Eliashberg theory and its application to superhydrides, Commun. Phys. 7, 33 (2024).
  65. H. Mori, T. Nomoto, R. Arita, and E. R. Margine, Efficient anisotropic Migdal-Eliashberg calculations with an intermediate representation basis and Wannier interpolation, Phys. Rev. B 110, 064505 (2024).
  66. W. L. McMillan, Transition temperature of strong-coupled superconductors, Phys. Rev. 167, 331 (1968).
  67. F. Marsiglio, Eliashberg theory: A short review, Ann. Phys. 417, 168102 (2020).
  68. E. Kogler, D. Spath, R. Lucrezi, H. Mori, Z. Zhu, Z. Li, E. R. Margine, and C. Heil, Isome: Streamlining high-precision Eliashberg calculations, Comput. Phys. Commun. 315, 109720 (2025).
  69. P. Morel and P. W. Anderson, Calculation of the superconducting state parameters with retarded electron-phonon interaction, Phys. Rev. 125, 1263 (1962).
  70. In the isome code [68], the Coulomb pseudopotential entering the Migdal–Eliashberg equations, μME*, is rescaled following Ref. [71]:1μME*=1μAD*+lnωphωc,where ωph is the characteristic cutoff frequency for the phonon-induced interaction and ωc is the Matsubara frequency cutoff.
  71. C. Pellegrini and A. Sanna, Ab initio methods for superconductivity, Nat. Rev. Phys. 6, 509 (2024).
  72. P. Anderson, Theory of dirty superconductors, J. Phys. Chem. Solids 11, 26 (1959).
  73. N. Takemori, R. Arita, and S. Sakai, Physical properties of weak-coupling quasiperiodic superconductors, Phys. Rev. B 102, 115108 (2020).
  74. Y. Nakajima, T. Nakagawa, T. Tamegai, and H. Harima, Specific-heat evidence for two-gap superconductivity in the ternary-iron silicide Lu2Fe3Si5, Phys. Rev. Lett. 100, 157001 (2008).
  75. J. Kačmarčík, Z. Pribulová, C. Marcenat, T. Klein, P. Rodière, L. Cario, and P. Samuely, Specific heat measurements of a superconducting NbS2 single crystal in an external magnetic field: Energy gap structure, Phys. Rev. B 82, 014518 (2010).
  76. A.-B. Chen and A. Sher, Semiconductor Alloys: Physics and Materials Engineering (Plenum Press, New York, 1995).
  77. P. Ferreira, R. Lucrezi, I. Guilhon, M. Marques, L. Teles, C. Heil, and L. Eleno, Ab initio modeling of superconducting alloys, Mater. Today Phys. 48, 101547 (2024).
  78. R. Dynes, McMillan's equation and the Tc of superconductors, Solid State Commun. 10, 615 (1972).
  79. P. B. Allen and R. C. Dynes, Transition temperature of strong-coupled superconductors reanalyzed, Phys. Rev. B 12, 905 (1975).
  80. P. Hohenberg and W. Kohn, Inhomogeneous electron gas, Phys. Rev. 136, B864 (1964).
  81. W. Kohn and L. J. Sham, Self-consistent equations including exchange and correlation effects, Phys. Rev. 140, A1133 (1965).
  82. P. Giannozzi, S. Baroni, N. Bonini, M. Calandra, R. Car, C. Cavazzoni, D. Ceresoli, G. L. Chiarotti, M. Cococcioni, I. Dabo, et al., QUANTUM ESPRESSO: A modular and open-source software project for quantum simulations of materials, J. Phys.: Condens. Matter 21, 395502 (2009).
  83. P. Giannozzi, O. Andreussi, T. Brumme, O. Bunau, M. B. Nardelli, M. Calandra, R. Car, C. Cavazzoni, D. Ceresoli, M. Cococcioni, et al., Advanced capabilities for materials modelling with QUANTUM ESPRESSO, J. Phys.: Condens. Matter 29, 465901 (2017).
  84. D. R. Hamann, Optimized norm-conserving Vanderbilt pseudopotentials, Phys. Rev. B 88, 085117 (2013).
  85. M. Schlipf and F. Gygi, Optimization algorithm for the generation of ONCV pseudopotentials, Comput. Phys. Commun. 196, 36 (2015).
  86. M. van Setten, M. Giantomassi, E. Bousquet, M. Verstraete, D. Hamann, X. Gonze, and G.-M. Rignanese, The PseudoDojo: Training and grading a 85 element optimized norm-conserving pseudopotential table, Comput. Phys. Commun. 226, 39 (2018).
  87. J. P. Perdew, K. Burke, and M. Ernzerhof, Generalized gradient approximation made simple, Phys. Rev. Lett. 77, 3865 (1996).
  88. H. J. Monkhorst and J. D. Pack, Special points for Brillouin-zone integrations, Phys. Rev. B 13, 5188 (1976).
  89. M. Methfessel and A. T. Paxton, High-precision sampling for Brillouin-zone integration in metals, Phys. Rev. B 40, 3616 (1989).
  90. S. Baroni, S. de Gironcoli, A. Dal Corso, and P. Giannozzi, Phonons and related crystal properties from density-functional perturbation theory, Rev. Mod. Phys. 73, 515 (2001).
  91. K. Bozier, K. Wang, B. Monserrat, and C. J. Pickard, High-throughput superconducting Tc predictions through density of states rescaling, Phys. Rev. B 113, 064507 (2026).
  92. A. Sher, M. van Schilfgaarde, A.-B. Chen, and W. Chen, Quasichemical approximation in binary alloys, Phys. Rev. B 36, 4279 (1987).
  93. K. Okhotnikov, T. Charpentier, and S. Cadars, Supercell program: A combinatorial structure-generation approach for the local-level modeling of atomic substitutions and partial occupancies in crystals, J. Cheminf. 8, 17 (2016).
  94. M. Kawamura, Fermisurfer: Fermi-surface viewer providing multiple representation schemes, Comput. Phys. Commun. 239, 197 (2019).
  95. K. Momma and F. Izumi, VESTA: A three-dimensional visualization system for electronic and structural analysis, J. Appl. Crystallogr. 41, 653 (2008).
  96. A. Kokalj, XCrySDen—a new program for displaying crystalline structures and electron densities, J. Mol. Graphics Modell. 17, 176 (1999).
  97. P. Nunes Ferreira, R. Lucrezi, S. Lee, L. Nathwani, M. Julian, R. Prasankumar, W. Pickett, C. Pickard, P. Kim, and C. Heil, First-principles evidence for conventional superconductivity in a quasicrystal approximant, Zenodo, 2025, https://doi.org/10.5281/zenodo.17589390.
  98. T. Takeuchi and U. Mizutani, Electronic structure, electron transport properties, and relative stability of icosahedral quasicrystals and their 1/1 and 2/1 approximants in the Al–Mg–Zn alloy system, Phys. Rev. B 52, 9300 (1995).

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