Starting from a microscopic Lieb-lattice model, the authors derive the nonlinear sigma model for altermagnetism, show its distinguishing Berry-phase term is perturbatively irrelevant in 2+1 dimensions, and compute the dynamical critical exponent from competing magnetic and Coulomb fluctuations.
Landau Theory of Altermagnetism
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abstract
We formulate a Landau theory for altermagnets, a class of colinear compensated magnets with spin-split bands. Starting from the non-relativistic limit, this Landau theory goes beyond a conventional analysis by including spin-space symmetries, providing a simple framework for understanding the key features of this family of materials. We find a set of multipolar secondary order parameters connecting existing ideas about the spin symmetries of these systems, their order parameters and the effect of non-zero spin-orbit coupling. We account for several features of canonical altermagnets such as RuO$_2$, MnTe and CuF$_2$ that go beyond symmetry alone, relating the order parameter to key observables such as magnetization, anomalous Hall conductivity and magneto-elastic and magneto-optical probes. Finally, we comment on generalizations of our framework to a wider family of exotic magnetic systems deriving from the zero spin-orbit coupled limit.
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Quantum critical scaling of altermagnetism
Starting from a microscopic Lieb-lattice model, the authors derive the nonlinear sigma model for altermagnetism, show its distinguishing Berry-phase term is perturbatively irrelevant in 2+1 dimensions, and compute the dynamical critical exponent from competing magnetic and Coulomb fluctuations.