Stripe antiferromagnetism in van der Waals metal HoTe3 decoupled from charge density wave order

Fuente: arXiv
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Autores principales: Yun, Weiyi, Nakano, Ryota, Misawa, Ryo, Yamada, Rinsuke, Akatsuka, Shun, Onuki, Yoshichika, Baral, Priya Ranjan, Saitoh, Hiraku, Kiyanagi, Ryoji, Ohhara, Takashi, Nakajima, Taro, Arima, Taka-hisa, Hirschberger, Max
Formato: Preprint
Publicado: 2026
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author Yun, Weiyi
Nakano, Ryota
Misawa, Ryo
Yamada, Rinsuke
Akatsuka, Shun
Onuki, Yoshichika
Baral, Priya Ranjan
Saitoh, Hiraku
Kiyanagi, Ryoji
Ohhara, Takashi
Nakajima, Taro
Arima, Taka-hisa
Hirschberger, Max
author_facet Yun, Weiyi
Nakano, Ryota
Misawa, Ryo
Yamada, Rinsuke
Akatsuka, Shun
Onuki, Yoshichika
Baral, Priya Ranjan
Saitoh, Hiraku
Kiyanagi, Ryoji
Ohhara, Takashi
Nakajima, Taro
Arima, Taka-hisa
Hirschberger, Max
contents The $R\mathrm{Te}_3$ ($R = \text{rare earth}$) family of layered van der Waals (vdW) compounds hosts coexisting magnetic and charge density wave (CDW) orders, yet the interplay between these degrees of freedom remains little explored. Combining polarized and unpolarized neutron diffraction on single-crystal $\mathrm{HoTe}_3$, we identify two distinct antiferromagnetic (AFM) phases, both exhibiting a collinear $\uparrow\uparrow\downarrow\downarrow$ motif within individual vdW layers. The two phases are distinguished by the vdW stacking of magnetic layers: ferromagnetic (FM) stacking in the higher-temperature AFM-II phase, here termed ``vertical-stripe'', and AFM stacking in the AFM-I ground state, here termed ``tilted-stripe''; the two phases have propagation vectors $\boldsymbol{q}_{\mathrm{m2}} = (0.48, 0, 0)$ and $\boldsymbol{q}_{\mathrm{m1}} = (0.5, 0.5, 0)$, respectively. In contrast to the CDW-driven exotic magnetism in $\mathrm{DyTe}_3$, $\mathrm{TbTe}_3$, and $\mathrm{GdTe}_3$, we find no evidence for coupling between magnetism and CDW in $\mathrm{HoTe}_3$. The relative alignment between AFM and CDW propagation vectors, as well as single-ion anisotropy, are likely essential for generating coupled spin/charge orders in layered vdW systems.
format Preprint
id arxiv_https___arxiv_org_abs_2602_16261
institution arXiv
publishDate 2026
record_format arxiv
spellingShingle Stripe antiferromagnetism in van der Waals metal HoTe3 decoupled from charge density wave order
Yun, Weiyi
Nakano, Ryota
Misawa, Ryo
Yamada, Rinsuke
Akatsuka, Shun
Onuki, Yoshichika
Baral, Priya Ranjan
Saitoh, Hiraku
Kiyanagi, Ryoji
Ohhara, Takashi
Nakajima, Taro
Arima, Taka-hisa
Hirschberger, Max
Strongly Correlated Electrons
Materials Science
The $R\mathrm{Te}_3$ ($R = \text{rare earth}$) family of layered van der Waals (vdW) compounds hosts coexisting magnetic and charge density wave (CDW) orders, yet the interplay between these degrees of freedom remains little explored. Combining polarized and unpolarized neutron diffraction on single-crystal $\mathrm{HoTe}_3$, we identify two distinct antiferromagnetic (AFM) phases, both exhibiting a collinear $\uparrow\uparrow\downarrow\downarrow$ motif within individual vdW layers. The two phases are distinguished by the vdW stacking of magnetic layers: ferromagnetic (FM) stacking in the higher-temperature AFM-II phase, here termed ``vertical-stripe'', and AFM stacking in the AFM-I ground state, here termed ``tilted-stripe''; the two phases have propagation vectors $\boldsymbol{q}_{\mathrm{m2}} = (0.48, 0, 0)$ and $\boldsymbol{q}_{\mathrm{m1}} = (0.5, 0.5, 0)$, respectively. In contrast to the CDW-driven exotic magnetism in $\mathrm{DyTe}_3$, $\mathrm{TbTe}_3$, and $\mathrm{GdTe}_3$, we find no evidence for coupling between magnetism and CDW in $\mathrm{HoTe}_3$. The relative alignment between AFM and CDW propagation vectors, as well as single-ion anisotropy, are likely essential for generating coupled spin/charge orders in layered vdW systems.
title Stripe antiferromagnetism in van der Waals metal HoTe3 decoupled from charge density wave order
topic Strongly Correlated Electrons
Materials Science
url https://arxiv.org/abs/2602.16261