Evidence of anisotropic three-dimensional weak localization in <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msub> <mml:mi>TiSe</mml:mi> <mml:mn>2</mml:mn> </mml:msub> </mml:math> nanoflakes

${\mathrm{TiSe}}_{2}$ 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 ${\mathrm{TiSe}}_{2}$ 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 ${\mathrm{TiSe}}_{2}$ flakes is most likely caused by the three-dimensional weak localization effect.

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Journal
Physical review. B./Physical review. B
Published
2025-10-02
DOI
https://doi.org/10.1103/mwfd-vhqd
Primary Topic
2D Materials and Applications
Type
article
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article

Evidence of anisotropic three-dimensional weak localization in <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msub> <mml:mi>TiSe</mml:mi> <mml:mn>2</mml:mn> </mml:msub> </mml:math> nanoflakes

Fan Yang, Guangtong Liu, Xiaocui Wang, Junxi Duan et al.
Physical review. B./Physical review. B
2D Materials and Applications
article

Evidence of anisotropic three-dimensional weak localization in <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msub> <mml:mi>TiSe</mml:mi> <mml:mn>2</mml:mn> </mml:msub> </mml:math> nanoflakes

Fan Yang, Guangtong Liu, Xiaocui Wang, Junxi Duan, Yang Yang, Lü Li, Zhiwei Wang, Yongkai Li
article en

Abstract

${\mathrm{TiSe}}_{2}$ 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 ${\mathrm{TiSe}}_{2}$ 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 ${\mathrm{TiSe}}_{2}$ flakes is most likely caused by the three-dimensional weak localization effect.

Physical review. B./Physical review. BVol. 112(16)
Beijing Institute of Technology (CN), Tianjin University (CN), Chinese Academy of Sciences (CN), Songshan Lake Materials Laboratory (CN), FZU ‒ Institute of Physics of the Academy of Sciences of the Czech Republic (CZ), Institute of Physics (CN), University of Chinese Academy of Sciences (CN)
Openalex Percentile: Top 73%
2D Materials and Applications
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