Resonant THz spectroscopy of Weyl semimetals

Accessing anomalous Weyl conductivity up to room
temperature in Weyl-Kondo semimetal CeCoGe3

CeCoGe3 is a material that has it all: It is a Weyl semimetal and a heavy-Fermion material, with three low-temperature antiferromagnetic transitions and pressure-induced superconductivity. What makes it specifically interesting in the THz range is that the strong correlations that lead to the hybridized Kondo state, actually push the Weyl nodal lines extremely close to the Fermi level. This brings the Weyl nodal lines within reach of resonant THz excitation. In this work, this is exploited to probe the anomalous electronic features associated with Weyl nodal lines with THz time-domain spectroscopy. Remarkably it is found that these features persist all the way up to room temperature and are not washed out by thermal broadening of electronic density of states. This is likely due to the extreme low-energy THz excitation towards these nodal lines. Within this energy range, no new electronic transitions appear even at room temperature, and the anomalous Weyl conductivity therefore remains protected.  
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Accessing anomalous Weyl conductivity up to roomtemperature in Weyl-Kondo semimetal CeCoGe3
2D THz spectroscopy of topological Kagome metal Mn3+xSn1-x across Weyl and Weyl-Kondo phase transitions

2D THz spectroscopy of topological Kagome metal Mn3+xSn1-x across Weyl and Weyl-Kondo phase transitions

Mn3Sn belongs to a new category of quantum materials known as topological Kagome metals (TKMs), characterized by a distinctive lattice geometry that gives rise to remarkable phenomena such as flat electronic bands and topological states. One especially compelling property of these materials is their capacity to host orbital currents, which are electron flows shaped not only by charge and spin, but also by the geometry and symmetry of the atomic orbitals themselves. Mn3Sn is therefore an ideal material building block for the emerging field of orbitronics. Here we used high-field 2D THz spectroscopy across a range of Mn3+xSn1-x stoichiometries, where this TKM transitions between paramagnetic, non-collinear antiferromagnetic states as well as a Weyl semimetal and possibly a Kondo-hybridized heavy Fermion state.
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