Altermagnetism combines aspects of both ferromagnetism and antiferromagnetism, breaking spin degeneracy while possessing no net magnetization. In this work, we study the symmetry requirements for topologically protected Weyl points in 2D altermagnets, involving bands with the same spin quantum number. We classify all spin-wallpaper groups whose symmetries protect 2D Weyl points and show that their nontrivial topology is charactrized by a quantized π-Berry phase. Representative electronic tight-binding and magnonic linear spin-wave models are constructed to investigate the unusual transport characteristics of these 2D Weyl points. Different mass terms, induced for example through strain or via coupling to light or a substrate, gap out the Weyl points leading to emerging gapped topological phases. Depending on the mass terms, these phases carry finite Chern and/or spin Chern numbers and exhibit protected edge states as well as anomalous electronic and thermal Hall responses. We calculate these Hall currents for the different topological phases.
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Parshukov et al. (2024) studied this question.
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