Temperature-dependent excitonic superfluid plasma frequency evolution in an excitonic insulator, Ta2NiSe5

Abstract An interesting van der Waals material, Ta2NiSe5 has been known one of strong excitonic insulator candidates since it has very small or zero bandgap and can have a strong exciton binding energy because of its quasi-one-dimensional crystal structure. Here we investigate a single crystal Ta2Ni...

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Autores principales: Yu-Seong Seo, Man Jin Eom, Jun Sung Kim, Chang-Jong Kang, Byung Il Min, Jungseek Hwang
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Publicado: Nature Portfolio 2018
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Acceso en línea:https://doaj.org/article/bdeb2a0a9ca944238fa0cd62ffc22873
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spelling oai:doaj.org-article:bdeb2a0a9ca944238fa0cd62ffc228732021-12-02T15:08:07ZTemperature-dependent excitonic superfluid plasma frequency evolution in an excitonic insulator, Ta2NiSe510.1038/s41598-018-30430-92045-2322https://doaj.org/article/bdeb2a0a9ca944238fa0cd62ffc228732018-08-01T00:00:00Zhttps://doi.org/10.1038/s41598-018-30430-9https://doaj.org/toc/2045-2322Abstract An interesting van der Waals material, Ta2NiSe5 has been known one of strong excitonic insulator candidates since it has very small or zero bandgap and can have a strong exciton binding energy because of its quasi-one-dimensional crystal structure. Here we investigate a single crystal Ta2NiSe5 using optical spectroscopy. Ta2NiSe5 has quasi-one-dimensional chains along the a-axis. We have obtained anisotropic optical properties of a single crystal Ta2NiSe5 along the a- and c-axes. The measured a- and c-axis optical conductivities exhibit large anisotropic electronic and phononic properties. With regard to the a-axis optical conductivity, a sharp peak near 3050 cm−1 at 9 K, with a well-defined optical gap ($${{\boldsymbol{\Delta }}}_{{\boldsymbol{o}}{\boldsymbol{p}}}^{{\boldsymbol{E}}{\boldsymbol{I}}}\,{\boldsymbol{\simeq }}$$ ΔopEI≃ 1800 cm−1) and a strong temperature-dependence, is observed. With an increase in temperature, this peak broadens and the optical energy gap closes around ∼325 K ($${{\boldsymbol{T}}}_{{\boldsymbol{c}}}^{{\boldsymbol{E}}{\boldsymbol{I}}}$$ TcEI ). The spectral weight redistribution with respect to the frequency and temperature indicates that the normalized optical energy gap $$({{\boldsymbol{\Delta }}}_{{\boldsymbol{o}}{\boldsymbol{p}}}^{{\boldsymbol{E}}{\boldsymbol{I}}}({\boldsymbol{T}})/\,{{\boldsymbol{\Delta }}}_{{\boldsymbol{o}}{\boldsymbol{p}}}^{{\boldsymbol{E}}{\boldsymbol{I}}}{\bf{(0)}})$$ (ΔopEI(T)/ΔopEI(0)) is $${\bf{1}}{\boldsymbol{-}}{({\boldsymbol{T}}/{{\boldsymbol{T}}}_{{\boldsymbol{c}}}^{{\boldsymbol{E}}{\boldsymbol{I}}})}^{{\bf{2}}}$$ 1−(T/TcEI)2 . The temperature-dependent superfluid plasma frequency of the excitonic condensation in Ta2NiSe5 has been determined from measured optical data. Our study may pave new avenues in the future research on excitonic insulators.Yu-Seong SeoMan Jin EomJun Sung KimChang-Jong KangByung Il MinJungseek HwangNature PortfolioarticleMedicineRScienceQENScientific Reports, Vol 8, Iss 1, Pp 1-9 (2018)
institution DOAJ
collection DOAJ
language EN
topic Medicine
R
Science
Q
spellingShingle Medicine
R
Science
Q
Yu-Seong Seo
Man Jin Eom
Jun Sung Kim
Chang-Jong Kang
Byung Il Min
Jungseek Hwang
Temperature-dependent excitonic superfluid plasma frequency evolution in an excitonic insulator, Ta2NiSe5
description Abstract An interesting van der Waals material, Ta2NiSe5 has been known one of strong excitonic insulator candidates since it has very small or zero bandgap and can have a strong exciton binding energy because of its quasi-one-dimensional crystal structure. Here we investigate a single crystal Ta2NiSe5 using optical spectroscopy. Ta2NiSe5 has quasi-one-dimensional chains along the a-axis. We have obtained anisotropic optical properties of a single crystal Ta2NiSe5 along the a- and c-axes. The measured a- and c-axis optical conductivities exhibit large anisotropic electronic and phononic properties. With regard to the a-axis optical conductivity, a sharp peak near 3050 cm−1 at 9 K, with a well-defined optical gap ($${{\boldsymbol{\Delta }}}_{{\boldsymbol{o}}{\boldsymbol{p}}}^{{\boldsymbol{E}}{\boldsymbol{I}}}\,{\boldsymbol{\simeq }}$$ ΔopEI≃ 1800 cm−1) and a strong temperature-dependence, is observed. With an increase in temperature, this peak broadens and the optical energy gap closes around ∼325 K ($${{\boldsymbol{T}}}_{{\boldsymbol{c}}}^{{\boldsymbol{E}}{\boldsymbol{I}}}$$ TcEI ). The spectral weight redistribution with respect to the frequency and temperature indicates that the normalized optical energy gap $$({{\boldsymbol{\Delta }}}_{{\boldsymbol{o}}{\boldsymbol{p}}}^{{\boldsymbol{E}}{\boldsymbol{I}}}({\boldsymbol{T}})/\,{{\boldsymbol{\Delta }}}_{{\boldsymbol{o}}{\boldsymbol{p}}}^{{\boldsymbol{E}}{\boldsymbol{I}}}{\bf{(0)}})$$ (ΔopEI(T)/ΔopEI(0)) is $${\bf{1}}{\boldsymbol{-}}{({\boldsymbol{T}}/{{\boldsymbol{T}}}_{{\boldsymbol{c}}}^{{\boldsymbol{E}}{\boldsymbol{I}}})}^{{\bf{2}}}$$ 1−(T/TcEI)2 . The temperature-dependent superfluid plasma frequency of the excitonic condensation in Ta2NiSe5 has been determined from measured optical data. Our study may pave new avenues in the future research on excitonic insulators.
format article
author Yu-Seong Seo
Man Jin Eom
Jun Sung Kim
Chang-Jong Kang
Byung Il Min
Jungseek Hwang
author_facet Yu-Seong Seo
Man Jin Eom
Jun Sung Kim
Chang-Jong Kang
Byung Il Min
Jungseek Hwang
author_sort Yu-Seong Seo
title Temperature-dependent excitonic superfluid plasma frequency evolution in an excitonic insulator, Ta2NiSe5
title_short Temperature-dependent excitonic superfluid plasma frequency evolution in an excitonic insulator, Ta2NiSe5
title_full Temperature-dependent excitonic superfluid plasma frequency evolution in an excitonic insulator, Ta2NiSe5
title_fullStr Temperature-dependent excitonic superfluid plasma frequency evolution in an excitonic insulator, Ta2NiSe5
title_full_unstemmed Temperature-dependent excitonic superfluid plasma frequency evolution in an excitonic insulator, Ta2NiSe5
title_sort temperature-dependent excitonic superfluid plasma frequency evolution in an excitonic insulator, ta2nise5
publisher Nature Portfolio
publishDate 2018
url https://doaj.org/article/bdeb2a0a9ca944238fa0cd62ffc22873
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