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Pressure-tuning topological phase transitions in Kagome superconductor CsTi$_3$Bi$_5$

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arxiv 2403.16119 v1 pith:NMVXFH5V submitted 2024-03-24 cond-mat.supr-con cond-mat.mtrl-sci

classification cond-mat.supr-concond-mat.mtrl-sci
keywords cstipressuresuperconductingkagomesuperconductivitytopologicalunderbehavior
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abstract

Recently, the Kagome metal CsTi$_3$Bi$_5$ has exhibited several novel quantum properties similar to CsV$_3$Sb$_5$, such as nontrivial topology, double-dome superconductivity, and flat band features. However, CsTi$_3$Bi$_5$ lacks the charge-density wave (CDW) present in CsV$_3$Sb$_5$, making the study of its emergence of double-dome superconductivity a focus of research. In this work, we have identified an order parameter, the three-band Z$_2$ topological index, that can describe the superconducting phase diagram of CsTi$_3$Bi$_5$ under pressure. Its evolution with pressure follows the expected behavior for superconductivity. Furthermore, the results of the Fermi surface under pressure reveal the potential presence of a Lifshitz transition in the vicinity of the vanishing point of the superconducting temperature change with pressure in CsTi$_3$Bi$_5$. These results indicate that the superconducting behavior of CsTi$_3$Bi$_5$ under pressure is caused by changes in the electronic structure leading to alterations in the topological properties, provide new insights and approaches for understanding the superconducting phenomenon in Kagome metals.

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  1. Interplay of $d$- and $p$-states in RbTi$_3$Bi$_5$ and CsTi$_3$Bi$_5$ flat-band kagome metals

    cond-mat.str-el 2025-01 conditional novelty 6.0 of 10

    Infrared spectroscopy with DFT shows that in RbTi3Bi5 and CsTi3Bi5, bismuth p-states contribute substantially to the low-energy optical response, correlations are strong, and a 150 K phonon plus localization-peak anom...

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