arXiv · 2110.13709
Topological phase transitions in strongly correlated systems: application to Co$_3$Sn$_2$S$_2$
Abstract
The topological transition in the strongly correlated half-metallic ferromagnetic compound Co$_3$Sn$_2$S$_2$ from Weyl semimetal (including chiral massless fermions) to a non-magnetic state is treated. This transition goes with a change in topological invariant, and is accompanied by a non-topological transition from saturated ferromagnetic to paramagnetic state, the minority Fermi surface being transformed from ghost (hidden) to real. A corresponding description is given in terms of slave fermion representation for the effective narrow-band Hubbard model. The system Co$_3$Sn$_2$S$_2$ provides a bright example of coexistence of non-trivial topology and strong low-dimensional ferromagnetism. A comparison is performed with other compounds where frustrations result in formation of a correlated paramagnetic state.
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V. Yu. Irkhin, Yu. N. Skryabin. 2021-10-26. Topological phase transitions in strongly correlated systems: application to Co$_3$Sn$_2$S$_2$. https://doi.org/10.1134/s0021364021210013
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