Cargando…

Superconducting, Topological, and Transport Properties of Kagome Metals CsTi(3)Bi(5) and RbTi(3)Bi(5)

The recently discovered ATi(3)Bi(5) (A=Cs, Rb) exhibit intriguing quantum phenomena including superconductivity, electronic nematicity, and abundant topological states. ATi(3)Bi(5) present promising platforms for studying kagome superconductivity, band topology, and charge orders in parallel with AV...

Descripción completa

Detalles Bibliográficos
Autores principales: Yi, Xin-Wei, Liao, Zheng-Wei, You, Jing-Yang, Gu, Bo, Su, Gang
Formato: Online Artículo Texto
Lenguaje:English
Publicado: AAAS 2023
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10543885/
https://www.ncbi.nlm.nih.gov/pubmed/37789987
http://dx.doi.org/10.34133/research.0238
_version_ 1785114381722320896
author Yi, Xin-Wei
Liao, Zheng-Wei
You, Jing-Yang
Gu, Bo
Su, Gang
author_facet Yi, Xin-Wei
Liao, Zheng-Wei
You, Jing-Yang
Gu, Bo
Su, Gang
author_sort Yi, Xin-Wei
collection PubMed
description The recently discovered ATi(3)Bi(5) (A=Cs, Rb) exhibit intriguing quantum phenomena including superconductivity, electronic nematicity, and abundant topological states. ATi(3)Bi(5) present promising platforms for studying kagome superconductivity, band topology, and charge orders in parallel with AV(3)Sb(5). In this work, we comprehensively analyze various properties of ATi(3)Bi(5) covering superconductivity under pressure and doping, band topology under pressure, thermal conductivity, heat capacity, electrical resistance, and spin Hall conductivity (SHC) using first-principles calculations. Calculated superconducting transition temperature (T(c)) of CsTi(3)Bi(5) and RbTi(3)Bi(5) at ambient pressure are about 1.85 and 1.92 K. When subject to pressure, T(c) of CsTi(3)Bi(5) exhibits a special valley and dome shape, which arises from quasi-two-dimensional compression to three-dimensional isotropic compression within the context of an overall decreasing trend. Furthermore, T(c) of RbTi(3)Bi(5) can be effectively enhanced up to 3.09 K by tuning the kagome van Hove singularities (VHSs) and flat band through doping. Pressures can also induce abundant topological surface states at the Fermi energy (E(F)) and tune VHSs across E(F). Additionally, our transport calculations are in excellent agreement with recent experiments, confirming the absence of charge density wave. Notably, SHC of CsTi(3)Bi(5) can reach up to 226ℏ ·(e· Ω ·cm)(–1) at E(F). Our work provides a timely and detailed analysis of the rich physical properties for ATi(3)Bi(5), offering valuable insights for further experimental verifications and investigations in this field.
format Online
Article
Text
id pubmed-10543885
institution National Center for Biotechnology Information
language English
publishDate 2023
publisher AAAS
record_format MEDLINE/PubMed
spelling pubmed-105438852023-10-03 Superconducting, Topological, and Transport Properties of Kagome Metals CsTi(3)Bi(5) and RbTi(3)Bi(5) Yi, Xin-Wei Liao, Zheng-Wei You, Jing-Yang Gu, Bo Su, Gang Research (Wash D C) Research Article The recently discovered ATi(3)Bi(5) (A=Cs, Rb) exhibit intriguing quantum phenomena including superconductivity, electronic nematicity, and abundant topological states. ATi(3)Bi(5) present promising platforms for studying kagome superconductivity, band topology, and charge orders in parallel with AV(3)Sb(5). In this work, we comprehensively analyze various properties of ATi(3)Bi(5) covering superconductivity under pressure and doping, band topology under pressure, thermal conductivity, heat capacity, electrical resistance, and spin Hall conductivity (SHC) using first-principles calculations. Calculated superconducting transition temperature (T(c)) of CsTi(3)Bi(5) and RbTi(3)Bi(5) at ambient pressure are about 1.85 and 1.92 K. When subject to pressure, T(c) of CsTi(3)Bi(5) exhibits a special valley and dome shape, which arises from quasi-two-dimensional compression to three-dimensional isotropic compression within the context of an overall decreasing trend. Furthermore, T(c) of RbTi(3)Bi(5) can be effectively enhanced up to 3.09 K by tuning the kagome van Hove singularities (VHSs) and flat band through doping. Pressures can also induce abundant topological surface states at the Fermi energy (E(F)) and tune VHSs across E(F). Additionally, our transport calculations are in excellent agreement with recent experiments, confirming the absence of charge density wave. Notably, SHC of CsTi(3)Bi(5) can reach up to 226ℏ ·(e· Ω ·cm)(–1) at E(F). Our work provides a timely and detailed analysis of the rich physical properties for ATi(3)Bi(5), offering valuable insights for further experimental verifications and investigations in this field. AAAS 2023-10-02 /pmc/articles/PMC10543885/ /pubmed/37789987 http://dx.doi.org/10.34133/research.0238 Text en Copyright © 2023 Xin-Wei Yi et al. https://creativecommons.org/licenses/by/4.0/Exclusive licensee Science and Technology Review Publishing House. No claim to original U.S. Government Works. Distributed under a Creative Commons Attribution License 4.0 (CC BY 4.0) (https://creativecommons.org/licenses/by/4.0/) .
spellingShingle Research Article
Yi, Xin-Wei
Liao, Zheng-Wei
You, Jing-Yang
Gu, Bo
Su, Gang
Superconducting, Topological, and Transport Properties of Kagome Metals CsTi(3)Bi(5) and RbTi(3)Bi(5)
title Superconducting, Topological, and Transport Properties of Kagome Metals CsTi(3)Bi(5) and RbTi(3)Bi(5)
title_full Superconducting, Topological, and Transport Properties of Kagome Metals CsTi(3)Bi(5) and RbTi(3)Bi(5)
title_fullStr Superconducting, Topological, and Transport Properties of Kagome Metals CsTi(3)Bi(5) and RbTi(3)Bi(5)
title_full_unstemmed Superconducting, Topological, and Transport Properties of Kagome Metals CsTi(3)Bi(5) and RbTi(3)Bi(5)
title_short Superconducting, Topological, and Transport Properties of Kagome Metals CsTi(3)Bi(5) and RbTi(3)Bi(5)
title_sort superconducting, topological, and transport properties of kagome metals csti(3)bi(5) and rbti(3)bi(5)
topic Research Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10543885/
https://www.ncbi.nlm.nih.gov/pubmed/37789987
http://dx.doi.org/10.34133/research.0238
work_keys_str_mv AT yixinwei superconductingtopologicalandtransportpropertiesofkagomemetalscsti3bi5andrbti3bi5
AT liaozhengwei superconductingtopologicalandtransportpropertiesofkagomemetalscsti3bi5andrbti3bi5
AT youjingyang superconductingtopologicalandtransportpropertiesofkagomemetalscsti3bi5andrbti3bi5
AT gubo superconductingtopologicalandtransportpropertiesofkagomemetalscsti3bi5andrbti3bi5
AT sugang superconductingtopologicalandtransportpropertiesofkagomemetalscsti3bi5andrbti3bi5