Emergent spin-resolved electronic charge density waves and pseudogap phenomena from strong $d$-wave altermagnetism

TL;DR

This paper models how strong d-wave altermagnetism in KV$_2$Se$_2$O leads to spin-resolved charge density waves and pseudogap phenomena, explaining experimental observations through a microscopic many-body approach.

Contribution

It introduces a self-consistent microscopic model showing how d-wave altermagnetism causes spin-resolved CDWs and pseudogaps, advancing understanding of metallic altermagnets.

Findings

Fermi surface reconstructs into spin-selective quasi-1D sheets.

Spin-resolved stripe phases form with orthogonal wave vectors.

Pseudogap regime persists above the density-wave transition temperature.

Abstract

Inspired by recent discovery of metallic $d$-wave altermagnetism in KV$_2$Se$_2$O, we develop a self-consistent microscopic many-body calculation of density-wave order for an itinerant altermagnetic metal. We show that the strong $d$-wave spin-momentum locking inherent to the altermagnetic band structure reconstructs the Fermi surface into spin-selective quasi-1D open sheets. This unique topology of Fermi surface drives an instability toward spin-resolved electronic charge density waves (CDWs), in which the ordering wave vectors for spin-up and spin-down electrons condense along two mutually orthogonal directions, forming spin-resolved stripe phases. As a consequence, this results in pronounced gap openings near the Fermi surface, and the superposition of these spin-resolved stripe orders leads to a checkerboard CDW in the charge channel and an antiphase spin-density-wave modulation in the spin channel. Upon increasing temperature, the density-wave order melts at $T_c$ due to thermal phase fluctuation while the gap opening persists, giving rise to a robust pseudogap regime, which eventually closes at a higher temperature $T_g$. The resulting simulations quantitatively reproduce the key features observed in the spectroscopic measurements, offering a consistent and generic understanding of the reported phenomena in KV$_2$Se$_2$O and, more broadly, in metallic altermagnets with strong spin-momentum locking.