Evidence of anisotropic three-dimensional weak-localization in TiSe nanoflakes
arXiv:2411.13488 · doi:10.1103/mwfd-vhqd
Abstract
TiSe is a typical transition-metal dichalcogenide known for its charge-density wave order. In this study, we report the observation of an unusual anisotropic negative magnetoresistance in exfoliated TiSe nanoflakes at low temperatures. Unlike the negative magnetoresistance reported in most other transition-metal dichalcogenides, our results cannot be explained by either the conventional two-dimensional weak localization effect or the Kondo effect. A comprehensive analysis of the data suggests that the observed anisotropic negative magnetoresistance in TiSe flakes is most likely caused by the three-dimensional weak localization effect. Our findings contribute to a deeper understanding of the phase-coherent transport processes in TiSe.
References in corpus (10)
- Orbital- and -selective hybridisation of Se 4p and Ti 3d states in the charge density wave phase of TiSe
- Signatures of the Kondo effect in VSe2
- Short-range phase coherence and origin of the 1T-TiSe2 charge density wave
- Fermi surface reconstruction and electron dynamics at the charge-density-wave transition in TiSe2
- Transition from semiconducting to metallic-like conducting and weak antilocalization effect in single crystals of LuPtSb
- On the origin of the anomalous peak in the resistivity of TiSe
- Preformed Excitons, Orbital Selectivity, and Charge-Density-Wave Order in 1T-TiSe_2
- Effect of synthesis conditions on the electrical resistivity of TiSe
- Intrinsic Insulating Ground State in Transition Metal Dichalcogenide TiSe2
- Anisotropic weakly localized transport in nitrogen-doped ultrananocrystalline diamond films