Symmetry as a Bridge Between Altermagnetism and Superconductivity
Tom G. Saunderson1
1. Institute of Physics, Martin-Luther University Halle-Wittenberg, D-06099 Halle (Saale), Germany
Since the discovery of cuprate high-Tc superconductivity, numerous theoretical frameworks have been proposed to explain its mechanism. Anderson’s RVB picture [1] and U(1) gauge theory [2], to name a few, motivate a minimal one-band view that largely integrates out oxygen. By contrast, altermagnetism [3] yields a d-wave-like k-space magnetic texture arising from alternatingly rotated non-magnetic cages, with La2CuO4 (the parent compound of a high-Tc cuprate) serving as a prototypical example.
As a proof of principle, in this talk I will show that in La2CuO4 an alternating local pairing potential on the two Cu sublattices (±s(r)) produces a nodal, d-wave-like Δ(k). Since orthorhombic tilts are not the driving mechanism—and in fact suppress superconductivity in nickelates [4] - I instead show that the in-plane oxygen sublattice of CuO2/NiO2 layers, ubiquitous in cuprates and nickelates, intrinsically realises the same symmetry. Imposing an oxygen-centred, staggered s-wave pairing yields a d-wave gap with perfect C4 symmetry, demonstrated self-consistently in NdNiO2 from first principles. While the microscopic mechanism driving this form of order remains unclear, I provide speculation on its possible origin. Moreover, this description of superconductivity enables a direct mapping of a real-space superconducting order parameter onto a lattice-based picture, allowing superconductivity and Hubbard-model physics to be treated on the same footing.
[1] Science 235, 1196–1198 (1987).
[2] Physical Review Letters 76, 503–506 (1996).
[3] Physical Review X 12, 040501 (2022).
[4] Nature 621, 493 (2023).
[5] T. G. Saunderson et al, arXiv:2509.06814 (2025)