Distinct switching of chiral transport in the kagome metals KV$_3$Sb$_5$ and CsV$_3$Sb$_5$

Fuente: arXiv
Guardado en:
Detalles Bibliográficos
Autores principales: Guo, Chunyu, van Delft, Maarten R., Gutierrez-Amigo, Martin, Chen, Dong, Putzke, Carsten, Wagner, Glenn, Fischer, Mark H., Neupert, Titus, Errea, Ion, Vergniory, Maia G., Wiedmann, Steffen, Felser, Claudia, Moll, Philip J. W.
Formato: Preprint
Publicado: 2023
Materias:
Acceso en línea:
Etiquetas: Agregar Etiqueta
Sin Etiquetas, Sea el primero en etiquetar este registro!
_version_ 1866929352897200128
author Guo, Chunyu
van Delft, Maarten R.
Gutierrez-Amigo, Martin
Chen, Dong
Putzke, Carsten
Wagner, Glenn
Fischer, Mark H.
Neupert, Titus
Errea, Ion
Vergniory, Maia G.
Wiedmann, Steffen
Felser, Claudia
Moll, Philip J. W.
author_facet Guo, Chunyu
van Delft, Maarten R.
Gutierrez-Amigo, Martin
Chen, Dong
Putzke, Carsten
Wagner, Glenn
Fischer, Mark H.
Neupert, Titus
Errea, Ion
Vergniory, Maia G.
Wiedmann, Steffen
Felser, Claudia
Moll, Philip J. W.
contents The kagome metals AV$_3$Sb$_5$ (A=K,Rb,Cs) present an ideal sandbox to study the interrelation between multiple coexisting correlated phases such as charge order and superconductivity. So far, no consensus on the microscopic nature of these states has been reached as the proposals struggle to explain all their exotic physical properties. Among these, field-switchable electric magneto-chiral anisotropy (eMChA) in CsV$_3$Sb$_5$ provides intriguing evidence for a rewindable electronic chirality, yet the other family members have not been likewise investigated. Here, we present a comparative study of magneto-chiral transport between CsV$_3$Sb$_5$ and KV$_3$Sb$_5$. Despite their similar electronic structure, KV$_3$Sb$_5$ displays negligible eMChA, if any, and with no field switchability. This is in stark contrast to the non-saturating eMChA in CsV$_3$Sb$_5$ even in high fields up to 35 T. In light of their similar band structures, the stark difference in eMChA suggests its origin in the correlated states. Clearly, the V kagome nets alone are not sufficient to describe the physics and the interactions with their environment are crucial in determining the nature of their low-temperature state.
format Preprint
id arxiv_https___arxiv_org_abs_2306_00593
institution arXiv
publishDate 2023
record_format arxiv
spellingShingle Distinct switching of chiral transport in the kagome metals KV$_3$Sb$_5$ and CsV$_3$Sb$_5$
Guo, Chunyu
van Delft, Maarten R.
Gutierrez-Amigo, Martin
Chen, Dong
Putzke, Carsten
Wagner, Glenn
Fischer, Mark H.
Neupert, Titus
Errea, Ion
Vergniory, Maia G.
Wiedmann, Steffen
Felser, Claudia
Moll, Philip J. W.
Strongly Correlated Electrons
Materials Science
The kagome metals AV$_3$Sb$_5$ (A=K,Rb,Cs) present an ideal sandbox to study the interrelation between multiple coexisting correlated phases such as charge order and superconductivity. So far, no consensus on the microscopic nature of these states has been reached as the proposals struggle to explain all their exotic physical properties. Among these, field-switchable electric magneto-chiral anisotropy (eMChA) in CsV$_3$Sb$_5$ provides intriguing evidence for a rewindable electronic chirality, yet the other family members have not been likewise investigated. Here, we present a comparative study of magneto-chiral transport between CsV$_3$Sb$_5$ and KV$_3$Sb$_5$. Despite their similar electronic structure, KV$_3$Sb$_5$ displays negligible eMChA, if any, and with no field switchability. This is in stark contrast to the non-saturating eMChA in CsV$_3$Sb$_5$ even in high fields up to 35 T. In light of their similar band structures, the stark difference in eMChA suggests its origin in the correlated states. Clearly, the V kagome nets alone are not sufficient to describe the physics and the interactions with their environment are crucial in determining the nature of their low-temperature state.
title Distinct switching of chiral transport in the kagome metals KV$_3$Sb$_5$ and CsV$_3$Sb$_5$
topic Strongly Correlated Electrons
Materials Science
url https://arxiv.org/abs/2306.00593