Origin of the charge density wave state in BaFe$_2$Al$_9$

Fuente: arXiv
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Auteurs principaux: Li, Yuping, Liu, Mingfeng, Li, Jiangxu, Wang, Jiantao, Lai, Junwen, He, Dongchang, Qiu, Ruizhi, Sun, Yan, Chen, Xing-Qiu, Liu, Peitao
Format: Preprint
Publié: 2024
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author Li, Yuping
Liu, Mingfeng
Li, Jiangxu
Wang, Jiantao
Lai, Junwen
He, Dongchang
Qiu, Ruizhi
Sun, Yan
Chen, Xing-Qiu
Liu, Peitao
author_facet Li, Yuping
Liu, Mingfeng
Li, Jiangxu
Wang, Jiantao
Lai, Junwen
He, Dongchang
Qiu, Ruizhi
Sun, Yan
Chen, Xing-Qiu
Liu, Peitao
contents Recently, a first-order phase transition associated with charge density wave (CDW) has been observed at low temperatures in intermetallic compound BaFe$_2$Al$_9$. However, this transition is absent in its isostructural sister compound BaCo$_2$Al$_9$. Consequently, an intriguing question arises as to the underlying factors that differentiate BaFe$_2$Al$_9$ from BaCo$_2$Al$_9$ and drive the CDW transition in BaFe$_2$Al$_9$. Here, we set out to address this question by conducting a comparative \emph{ab initio} study of the electronic structures, lattice dynamics, \textcolor{black}{and electron-phonon interactions} of their high-temperature phases. We find that both compounds are dynamically stable with similar phonon dispersions. The electronic structure calculations reveal that both compounds are nonmagnetic metals; however, they exhibit distinct band structures around the Fermi level. In particular, BaFe$_2$Al$_9$ exhibits a higher density of states at the Fermi level with dominant partially filled Fe-$3d$ states and a more intricate Fermi surface. This leads to an electronic instability of BaFe$_2$Al$_9$ toward the CDW transition, which is manifested by the diverged electronic susceptibility at the CDW wave vector $\mathbf{q}_{\rm CDW}$=(0.5, 0, 0.3), observable in both the real and imaginary parts. Conversely, BaCo$_2$Al$_9$ does not display such behavior, aligning well with experimental observations. Although the electron-phonon interactions in BaFe$_2$Al$_9$ surpass those in BaCo$_2$Al$_9$ by two orders of magnitude, the strength is relatively weak at the CDW wave vector, suggesting that the CDW in BaFe$_2$Al$_9$ is primarily driven by electronic factors.
format Preprint
id arxiv_https___arxiv_org_abs_2410_22734
institution arXiv
publishDate 2024
record_format arxiv
spellingShingle Origin of the charge density wave state in BaFe$_2$Al$_9$
Li, Yuping
Liu, Mingfeng
Li, Jiangxu
Wang, Jiantao
Lai, Junwen
He, Dongchang
Qiu, Ruizhi
Sun, Yan
Chen, Xing-Qiu
Liu, Peitao
Materials Science
Recently, a first-order phase transition associated with charge density wave (CDW) has been observed at low temperatures in intermetallic compound BaFe$_2$Al$_9$. However, this transition is absent in its isostructural sister compound BaCo$_2$Al$_9$. Consequently, an intriguing question arises as to the underlying factors that differentiate BaFe$_2$Al$_9$ from BaCo$_2$Al$_9$ and drive the CDW transition in BaFe$_2$Al$_9$. Here, we set out to address this question by conducting a comparative \emph{ab initio} study of the electronic structures, lattice dynamics, \textcolor{black}{and electron-phonon interactions} of their high-temperature phases. We find that both compounds are dynamically stable with similar phonon dispersions. The electronic structure calculations reveal that both compounds are nonmagnetic metals; however, they exhibit distinct band structures around the Fermi level. In particular, BaFe$_2$Al$_9$ exhibits a higher density of states at the Fermi level with dominant partially filled Fe-$3d$ states and a more intricate Fermi surface. This leads to an electronic instability of BaFe$_2$Al$_9$ toward the CDW transition, which is manifested by the diverged electronic susceptibility at the CDW wave vector $\mathbf{q}_{\rm CDW}$=(0.5, 0, 0.3), observable in both the real and imaginary parts. Conversely, BaCo$_2$Al$_9$ does not display such behavior, aligning well with experimental observations. Although the electron-phonon interactions in BaFe$_2$Al$_9$ surpass those in BaCo$_2$Al$_9$ by two orders of magnitude, the strength is relatively weak at the CDW wave vector, suggesting that the CDW in BaFe$_2$Al$_9$ is primarily driven by electronic factors.
title Origin of the charge density wave state in BaFe$_2$Al$_9$
topic Materials Science
url https://arxiv.org/abs/2410.22734