Unconventional insulator-to-metal phase transition in Mn<sub>3</sub>Si<sub>2</sub>Te<sub>6</sub>.
basic_science · Level V
Where this comes from
- Record sourced from PubMed, PMID 39285185.
- Also identified by DOI 10.1038/s41467-024-52350-1 and PMC identifier 11405877.
- Licence recorded as CC BY-NC-ND.
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Abstract
The nodal-line semiconductor Mn<sub>3</sub>Si<sub>2</sub>Te<sub>6</sub> is generating enormous excitment due to the recent discovery of a field-driven insulator-to-metal transition and associated colossal magnetoresistance as well as evidence for a new type of quantum state involving chiral orbital currents. Strikingly, these qualities persist even in the absence of traditional Jahn-Teller distortions and double-exchange mechanisms, raising questions about exactly how and why magnetoresistance occurs along with conjecture as to the likely signatures of loop currents. Here, we measured the infrared response of Mn<sub>3</sub>Si<sub>2</sub>Te<sub>6</sub> across the magnetic ordering and field-induced insulator-to-metal transitions in order to explore colossal magnetoresistance in the absence of Jahn-Teller and double-exchange interactions. Rather than a traditional metal with screened phonons, the field-driven insulator-to-metal transition leads to a weakly metallic state with localized carriers. Our spectral data are fit by a percolation model, providing evidence for electronic inhomogeneity and phase separation. Modeling also reveals a frequency-dependent threshold field for carriers contributing to colossal magnetoresistance which we discuss in terms of polaron formation, chiral orbital currents, and short-range spin fluctuations. These findings enhance the understanding of insulator-to-metal transitions in new settings and open the door to the design of unconventional colossal magnetoresistant materials.