Pith. sign in

Title resolution pending

When α = 0,β ̸= 0, F ss′ 0β (k, k + q) = 1 2 (sˆdβ k+q + s′ ˆdβ k + iss′ X ij ϵβji ˆdi k+q ˆdj k) = 1 2 [sˆdβ k+q + s′ ˆdβ k + iss′(ˆdk × ˆdk+q)β]

1 Pith paper cite this work. Polarity classification is still indexing.

1 Pith paper citing it
browse 1 citing papers

Title metadata for this work has not finished resolving. The hub is built from the citation graph; the title resolver retries DOI and OpenAlex on its next pass.

fields

cond-mat.str-el 1

years

2024 1

verdicts

CONDITIONAL 1

representative citing papers

Quasiparticle interference in altermagnets

cond-mat.str-el · 2024-11-26 · conditional · novelty 6.0

Spin-resolved quasiparticle interference in d-wave altermagnets yields channel-specific real and imaginary Fourier patterns that map the Fermi surface and can distinguish Zeeman splitting from Rashba spin-orbit coupling.

citing papers explorer

Showing 1 of 1 citing paper.

  • Quasiparticle interference in altermagnets cond-mat.str-el · 2024-11-26 · conditional · none · ref 2

    Spin-resolved quasiparticle interference in d-wave altermagnets yields channel-specific real and imaginary Fourier patterns that map the Fermi surface and can distinguish Zeeman splitting from Rashba spin-orbit coupling.