No observation of chiral flux current in the topological kagome metal <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:msub><mml:mi mathvariant="normal">CsV</mml:mi><mml:mn>3</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">Sb</mml:mi><mml:mn>5</mml:mn></mml:msub></mml:math>

Huazhou Li(Collaborative Innovation Center of Advanced Microstructures), Siyuan Wan(Collaborative Innovation Center of Advanced Microstructures), Han Li(Collaborative Innovation Center of Advanced Microstructures), Qing Li(Collaborative Innovation Center of Advanced Microstructures), Qiangqiang Gu(Collaborative Innovation Center of Advanced Microstructures), Huan Yang(Collaborative Innovation Center of Advanced Microstructures), Yongkai Li(Beijing Institute of Technology), Zhiwei Wang(Beijing Institute of Technology), Yugui Yao(Beijing Institute of Technology), Hai‐Hu Wen(Collaborative Innovation Center of Advanced Microstructures)
Physical review. B./Physical review. B
January 3, 2022
Cited by 67Open Access
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Abstract

Compounds with kagome lattice usually host many exotic quantum states, including the quantum spin liquid, non-trivial topological Dirac bands and a strongly renormalized flat band, etc. Recently an interesting vanadium based kagome family $A{\mathrm{V}}_{3}{\mathrm{Sb}}_{5}$ $(A=\mathrm{K},\mathrm{Rb},\text{or}\phantom{\rule{0.28em}{0ex}}\mathrm{Cs})$ was discovered, and these materials exhibit multiple interesting properties, including unconventional saddle-point driving charge density wave (CDW) state, superconductivity, etc. Furthermore, some experiments show the anomalous Hall effect which inspires us to believe that there might be some chiral flux current states. Here we report scanning tunneling measurements by using spin-polarized tips. Although we have observed clearly the $2{a}_{0}\ifmmode\times\else\texttimes\fi{}2{a}_{0}$ CDW and $4{a}_{0}$ stripe orders, the well-designed experiments with refined spin-polarized tips do not reveal any trace of the chiral flux current phase in ${\mathrm{CsV}}_{3}{\mathrm{Sb}}_{5}$ within the limits of experimental accuracy. No observation of the local magnetic moment in our experiments may put an upper bound constraint on the magnitude of magnetic moments induced by the possible chiral loop current which has a time-reversal symmetry breaking along $c$ axis in ${\mathrm{CsV}}_{3}{\mathrm{Sb}}_{5}$.


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