Altermagnetism is a collinear magnetic order in which opposite spin species are exchanged under a real-space rotation. Hence, the search for physical realizations has focused on crystalline solids with specific rotational symmetry. Here, we show that altermagnetism can also emerge in noncrystalline systems, such as amorphous solids, despite the lack of global rotational symmetries. We construct a minimal Hamiltonian with two directional orbitals per site on an amorphous lattice with interactions that are invariant under spin rotation. Altermagnetism then arises due to spontaneous symmetry breaking in the spin and orbital degrees of freedom around each atom, displaying a common point group symmetry. This form of altermagnetism exhibits anisotropic spin transport and spin spectral functions, both experimentally measurable. Our mechanism generalizes to any lattice and any altermagnetic order, opening the search for altermagnetic phenomena to noncrystalline systems.

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• Altermagnetism
• Orbital order
• Altermagnets
• Amorphous materials
• Mean field theory
• Tight-binding model