Reuse & Permissions

It is not necessary to obtain permission to reuse this article or its components as it is available under the terms of the Creative Commons Attribution 4.0 International license. This license permits unrestricted use, distribution, and reproduction in any medium, provided attribution to the author(s) and the published article's title, journal citation, and DOI are maintained. Please note that some figures may have been included with permission from other third parties. It is your responsibility to obtain the proper permission from the rights holder directly for these figures.

Export citation

Export citation

Choose format for download:

Download Citation
  • Open Access

An ab Initio Answer to Long-Debated Questions about Superconducting Nb3Sn

Alessio Cucciari* and Lilia Boeri†

  • *Contact author: alessio.cucciari@uniroma1.it
  • †Contact author: lilia.boeri@uniroma1.it

PRX Energy 5, 013006 – Published 4 February, 2026

DOI: https://doi.org/10.1103/dmwh-1sbf

Abstract

Nb3Sn is the workhorse superconductor for high-field applications; however, several fundamental aspects remain open 70 years after its discovery. Using anharmonic ab initio Migdal-Eliashberg theory, we resolve three key questions: (1) the cubic-to-tetragonal martensitic transition is weakly first order; (2) the superconducting gap is strongly anisotropic but continuous over the Fermi surface; and (3) the drop of Hc2 across the transition arises from both reduced electron-phonon coupling and a redistribution of Fermi velocities. The orbital origin of the gap anisotropy suggests targeted doping strategies: Sn-site substitution can increase both Tc and Hc2, while Nb-site substitution raises Hc2 at the cost of lowering Tc.

View figure in article

Physics Subject Headings (PhySH)

Popular Summary

Article Text

Supplemental Material

References (81)

  1. D. Larbalestier, A. Gurevich, D. M. Feldmann, and A. Polyanskii, High-Tc superconducting materials for electric power applications, Nature 414, 368 (2001).
  2. A. Godeke, A review of the properties of Nb3Sn and their variation with A15 composition, morphology and strain state, Supercond. Sci. Technol. 19, R68 (2006).
  3. C. Yao and Y. Ma, Superconducting materials: Challenges and opportunities for large-scale applications, iScience 24, 102541 (2021).
  4. G. Stewart, Superconductivity in the A15 structure, Phys. C: Supercond. Appl. 514, 28 (2015).
  5. D. Dew-Hughes, Superconducting A-15 compounds: A review, Cryogenics 15, 435 (1975).
  6. G. Shirane and J. D. Axe, Neutron scattering study of the lattice-dynamical phase transition in Nb3Sn, Phys. Rev. B 4, 2957 (1971).
  7. R. N. Bhatt and W. L. McMillan, Landau theory of the martensitic transition in A-15 compounds, Phys. Rev. B 14, 1007 (1976).
  8. Y. Fujii, J. B. Hastings, M. Kaplan, G. Shirane, Y. Inada, and N. Kitamura, Study of the tetragonal-to-tetragonal phase transition of the A15 pseudobinary alloy Nb3Sn1−xSbx by neutron and x-ray scattering, Phys. Rev. B 25, 364 (1982).
  9. L. R. Testardi, Structural instability and superconductivity in A-15 compounds, Rev. Mod. Phys. 47, 637 (1975).
  10. K. Tachikawa, H. Sekine, and Y. Iijima, Composite-processed Nb3Sn with titanium addition to the matrix, J. Appl. Phys. 53, 5354 (1982).
  11. R. Flükiger, C. Senatore, M. Cesaretti, F. Buta, D. Uglietti, and B. Seeber, Optimization of Nb3Sn and MgB2 wires, Superconductor Science and Technology 21, 054015 (2008).
  12. S. M. Heald, C. Tarantini, P. J. Lee, M. D. Brown, Z. Sung, A. K. Ghosh, and D. C. Larbalestier, Evidence from EXAFS for different Ta/Ti site occupancy in high critical current density Nb3Sn superconductor wires, Sci. Rep. 8, 4798 (2018).
  13. C. Tarantini, F. Kametani, S. Balachandran, S. M. Heald, L. Wheatley, C. R. M. Grovenor, M. P. Moody, Y.-F. Su, P. J. Lee, and D. C. Larbalestier, Origin of the enhanced Nb3Sn performance by combined Hf and Ta doping, Sci. Rep. 11, 17845 (2021).
  14. L. Boeri, R. Hennig, P. Hirschfeld, G. Profeta, A. Sanna, E. Zurek, W. E. Pickett, M. Amsler, R. Dias, M. I. Eremets et al., The 2021 room-temperature superconductivity roadmap, J. Phys.: Condens. Matter 34, 183002 (2022).
  15. A. Cucciari, D. Naddeo, S. Di Cataldo, and L. Boeri, NbTi: A nontrivial puzzle for the conventional theory of superconductivity, Phys. Rev. B 110, L140502 (2024).
  16. B. Sadigh and V. Ozoliņš, Structural instability and electronic excitations in Nb3Sn, Phys. Rev. B 57, 2793 (1998).
  17. B. M. Klein and Z. Lu, Structural instabilities in A15 materials driven by anharmonic phonons: A first-principles study, Phys. B: Condens. Matter 296, 120 (2001).
  18. H. M. Tütüncü, G. P. Srivastava, S. Bağcı, and S. Duman, Theoretical examination of whether phonon dispersion in Nb3Sn is anomalous, Phys. Rev. B 74, 212506 (2006).
  19. G. De Marzi, L. Morici, L. Muzzi, A. della Corte, and M. Buongiorno Nardelli, Strain sensitivity and superconducting properties of Nb3Sn from first principles calculations, J. Phys.: Condens. Matter 25, 135702 (2013).
  20. R. Zhang, P. Gao, X. Wang, and Y. Zhou, First-principles study on elastic and superconducting properties of Nb3Sn and Nb3Al under hydrostatic pressure, AIP Adv. 5, 107233 (2015).
  21. F. Gala, G. De Marzi, L. Muzzi, and G. Zollo, The role of stoichiometry in superconducting Nb1−βSnβ: Electronic and vibrational properties from ab initio calculations, Phys. Chem. Chem. Phys. 18, 32840 (2016).
  22. X. Yang, Q. Du, L. Qiao, G. Xiao, Z. Li, and L. Yang, Microscopic origin of the abnormal elastic behavior accompanying the superconducting transition in Nb3Sn crystals: An extended ab initio study, J. Alloys Compd. 941, 168891 (2023).
  23. L.-N. Wu, S.-T. Yang, J.-K. Shen, J.-S. Zhang, and F.-H. Liu, Coexistence of superconductivity and charge density wave instability in A15-Nb3Sn, Phys. Chem. Chem. Phys. 25, 32452 (2023).
  24. W. Chen, X. Chen, Y. Gao, Y. Zhou, S. Cai, J. Zhao, K. Yang, A. Li, S. Jiang, Q. Wu et al., Evolution of superconductivity and corresponding electronic structure in pressurized Nb3Sn, Superconductivity 13, 100153 (2025).
  25. L. Monacelli, R. Bianco, M. Cherubini, M. Calandra, I. Errea, and F. Mauri, The stochastic self-consistent harmonic approximation: Calculating vibrational properties of materials with full quantum and anharmonic effects, J. Phys. Condens. Matter 33, 363001 (2021).
  26. 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).
  27. 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).
  28. P. W. Anderson and E. I. Blount, Symmetry considerations on martensitic transformations: “Ferroelectric” metals? Phys. Rev. Lett. 14, 217 (1965).
  29. B. W. Batterman and C. S. Barrett, Crystal structure of superconducting V3Si, Phys. Rev. Lett. 13, 390 (1964).
  30. L. Vieland and A. Wicklund, Specific heat and the lattice transformation in Nb3Sn, Solid State Commun. 7, 37 (1969).
  31. R. Mailfert, B. Batterman, and J. Hanak, Low temperature structural transformation in Nb3Sn, Phys. Lett. A 24, 315 (1967).
  32. R. Escudero, F. Morales, and S. Bernès, Specific heat studies of pure Nb3Sn single crystals at low temperature, J. Phys.: Condens. Matter 21, 325701 (2009).
  33. M. Acosta-Alejandro, J. Lezama-Pacheco, R. Falconi, R. Escudero, and J. Mustre de León, Local structure instability across the martensitic transition in Nb3Sn, J. Supercond. Novel Magn. 24, 1219 (2011).
  34. V. Guritanu, W. Goldacker, F. Bouquet, Y. Wang, R. Lortz, G. Goll, and A. Junod, Specific heat of Nb3Sn: The case for a second energy gap, Phys. Rev. B 70, 184526 (2004).
  35. M. Marz, G. Goll, W. Goldacker, and R. Lortz, Second superconducting energy gap of Nb3Sn observed by breakjunction point-contact spectroscopy, Phys. Rev. B 82, 024507 (2010).
  36. Y. J. Jo, J. Zhou, Z. H. Sung, P. J. Lee, and D. C. Larbalestier, Specific heat of Nb3Sn: The case for a single gap, APL Mater. 2, 106101 (2014).
  37. J. Zhou, Y. Jo, Z. Hawn Sung, H. Zhou, P. J. Lee, and D. C. Larbalestier, Evidence that the upper critical field of Nb3Sn is independent of whether it is cubic or tetragonal, Appl. Phys. Lett. 99, 122507 (2011).
  38. J. P. Perdew, A. Ruzsinszky, G. I. Csonka, O. A. Vydrov, G. E. Scuseria, L. A. Constantin, X. Zhou, and K. Burke, Restoring the density-gradient expansion for exchange in solids and surfaces, Phys. Rev. Lett. 100, 136406 (2008).
  39. See Supplemental Material at http://link.aps.org/supplemental/10.1103/dmwh-1sbf for further computational details on the ab initio calculations, as well as additional figures for convergence tests, electronic structure and Fermi-surface analysis, SSCHA convergence, and MLIP training.
  40. S. Schicktanz, R. Kaiser, E. Schneider, and W. Gläser, Raman studies of A15 compounds, Phys. Rev. B 22, 2386 (1980).
  41. P. Jin, L. Li, X. Li, Q. Wang, and J. Cheng, Residual stress in Nb3Sn superconductor strand introduced by structure and stoichiometric distribution after heat treatment, IEEE Trans. Appl. Supercond. 27, 1 (2017).
  42. J. Lee, S. Posen, Z. Mao, Y. Trenikhina, K. He, D. L. Hall, M. Liepe, and D. N. Seidman, Atomic-scale analyses of Nb3Sn on Nb prepared by vapor diffusion for superconducting radiofrequency cavity applications: A correlative study, Supercond. Sci. Technol. 32, 024001 (2019).
  43. It is worth noting that the energy differences involved are so small that we cannot exclude the possibility that other effects could reshape the Born-Oppenheimer surface and stabilize a tetragonal phase. Indeed, test calculations using the PBE0 hybrid functional [81] predict a larger energy gain (approximately 5 meV/atom) for the experimental tetragonal structure over the cubic phase, at least at the harmonic level.
  44. L. Boeri, G. Bachelet, E. Cappelluti, and L. Pietronero, Small Fermi energy and phonon anharmonicity in MgB2 and related compounds, Phys. Rev. B 65, 214501 (2002).
  45. J. D. Axe and G. Shirane, Inelastic-neutron-scattering study of acoustic phonons in Nb3Sn, Phys. Rev. B 8, 1965 (1973).
  46. L. Pintschovius, H. G. Smith, N. Wakabayashi, W. Reichardt, W. Weber, G. W. Webb, and Z. Fisk, Lattice dynamics of the A15 compound Nb3Sb, Phys. Rev. B 28, 5866 (1983).
  47. L. Pintschovius, H. Takei, and N. Toyota, Phonon anomalies in Nb3Sn, Phys. Rev. Lett. 54, 1260 (1985).
  48. L. Y. L. Shen, Tunneling into a high - Tc superconductor-Nb3Sn, Phys. Rev. Lett. 29, 1082 (1972).
  49. D. A. Rudman and M. R. Beasley, Microscopic superconducting parameters from tunneling in A15 Nb-Sn, Phys. Rev. B 30, 2590 (1984).
  50. J. K. Freericks, A. Y. Liu, A. Quandt, and J. Geerk, Nonconstant electronic density of states tunneling inversion for A15 superconductors: Nb3Sn, Phys. Rev. B 65, 224510 (2002).
  51. G. Kieselmann and H. Rietschel, On the analysis of tunneling data for A15 superconductors, J. Low Temp. Phys. 46, 27 (1982).
  52. E. L. Wolf, Principles of Electron Tunneling Spectroscopy (Oxford University Press, 2011), ISBN: 9780199589494.
  53. J. Geerk, U. Schneider, W. Bangert, H. Rietschell, F. Gompf, M. Gurvitch, J. Remeika, and J. Rowell, Electron tunneling into A15 and B1 superconductors, Phys. B+C 135, 187 (1985).
  54. M. Mentink, M. Dhalle, D. Dietderich, A. Godeke, F. Hellman, and H. T. Kate, The effects of disorder on the normal state and superconducting properties of Nb3Sn, Supercond. Sci. Technol. 30, 025006 (2017).
  55. H. Lee, S. Poncé, K. Bushick, S. Hajinazar, J. Lafuente-Bartolome, J. Leveillee, C. Lian, J.-M. Lihm, F. Macheda, H. Mori et al., Electron-phonon physics from first principles using the EPW code, npj Comput. Mater. 9, 156 (2023).
  56. P. Morel and P. W. Anderson, Calculation of the superconducting state parameters with retarded electron-phonon interaction, Phys. Rev. 125, 1263 (1962).
  57. C. Pellegrini, C. Kukkonen, and A. Sanna, Ab initio calculations of superconducting transition temperatures: When going beyond RPA is essential, Phys. Rev. B 108, 064511 (2023).
  58. J. P. Charlesworth, I. Macphail, and P. E. Madsen, Experimental work on the niobium-tin constitution diagram and related studies, J. Mater. Sci. 5, 580 (1970).
  59. A. Sanna, C. Pellegrini, and E. K. U. Gross, Combining Eliashberg theory with density functional theory for the accurate prediction of superconducting transition temperatures and gap functions, Phys. Rev. Lett. 125, 057001 (2020).
  60. T. P. Orlando, E. J. McNiff, S. Foner, and M. R. Beasley, Critical fields, Pauli paramagnetic limiting, and material parameters of Nb3Sn and V3Si, Phys. Rev. B 19, 4545 (1979).
  61. E. Helfand and N. R. Werthamer, Temperature and purity dependence of the superconducting critical field, Hc2. II, Phys. Rev. 147, 288 (1966).
  62. Our calculations refer to ideal stoichiometric crystals and do not include extrinsic effects such as inhomogeneity or residual cubic domains, which may justify why the experimentally observed Tc reduction (typically 1 K) is much smaller than the correspondent Hc2 reduction.
  63. L. J. Vieland and R. W. Cohen, Study of Transition Temperature in Superconductors, Final Report NAS 8-21384 (RCA Laboratories, Princeton, New Jersey 08540, 1970) prepared for NASA under Contract No. NAS 8-21384, reporting period: 11 March 1968 to 10 March 1970.
  64. C. Tresca, G. Profeta, G. Marini, G. B. Bachelet, A. Sanna, M. Calandra, and L. Boeri, Why mercury is a superconductor, Phys. Rev. B 106, L180501 (2022).
  65. N. S. Sitaraman, Z. Sun, B. L. Francis, A. C. Hire, T. Oseroff, Z. Baraissov, T. A. Arias, R. G. Hennig, M. U. Liepe, D. A. Muller, and M. K. Transtrum (Center for Bright Beams), Enhanced surface superconductivity of niobium by zirconium doping, Phys. Rev. Appl. 20, 014064 (2023).
  66. S. D. Cataldo, W. Cursio, and L. Boeri, Vacancy-controlled superconductivity in rock-salt carbides: Towards predictive modelling of real-world superconductors, arXiv:2506.07768.
  67. E. Kogler, M. R. Sahoo, C.-N. Tsai, F. Jöbstl, R. Lucrezi, P. I. C. Cooke, B. Kunert, R. Resel, C. J. Pickard, M. N. Julian et al., Vacancy-free cubic superconducting NbN enabled by quantum anharmonicity, Commun. Mater. 6, 283 (2025).
  68. D. Jones, A. Östlin, A. Chmeruk, F. Beiuşeanu, U. Eckern, L. Vitos, and L. Chioncel, Quasiparticle Fermi surfaces of niobium and niobium-titanium alloys at high pressure, Phys. Rev. B 111, 165152 (2025).
  69. W. Weber and L. F. Mattheiss, Electronic structure of tetragonal Nb3Sn, Phys. Rev. B 25, 2270 (1982).
  70. S. Baroni, S. de Gironcoli, A. D. Corso, and P. Giannozzi, Phonons and related crystal properties from density-functional perturbation theory, Rev. Mod. Phys 73, 515 (2001).
  71. 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).
  72. D. R. Hamann, Optimized norm-conserving Vanderbilt pseudopotentials, Phys. Rev. B 88, 085117 (2013).
  73. H. J. Monkhorst and J. D. Pack, Special points for Brillouin-zone integrations, Phys. Rev. B 13, 5188 (1976).
  74. M. Methfessel and A. T. Paxton, High-precision sampling for Brillouin-zone integration in metals, Phys. Rev. B 40, 3616 (1989).
  75. I. Errea, M. Calandra, and F. Mauri, Anharmonic free energies and phonon dispersions from the stochastic self-consistent harmonic approximation: Application to platinum and palladium hydrides, Phys. Rev. B 89, 064302 (2014).
  76. I. Novoselov, A. Yanilkin, A. Shapeev, and E. Podryabinkin, Moment tensor potentials as a promising tool to study diffusion processes, Comput. Mater. Sci. 164, 46 (2019).
  77. 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).
  78. I. S. Novikov, K. Gubaev, E. V. Podryabinkin, and A. V. Shapeev, The MLIP package: Moment tensor potentials with MPI and active learning, Mach. Learn.: Sci. Technol. 2, 025002 (2021).
  79. V. L. Deringer, M. A. Caro, and G. Csányi, Machine learning interatomic potentials as emerging tools for materials science, Adv. Mater. 31, 1902765 (2019).
  80. A. Cucciari and L. Boeri, Dataset supporting “An ab initio answer to long-debated questions about superconducting Nb3Sn”, Zenodo, 2026, https://doi.org/10.5281/zenodo.18226137.
  81. J. P. Perdew, M. Ernzerhof, and K. Burke, Rationale for mixing exact exchange with density functional approximations, J. Chem. Phys. 105, 9982 (1996).

Outline

Information

Sign In to Your Journals Account

Filter

Filter

Article Lookup

Enter a citation