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arXiv 2608.29116cond-mat.str-elcond-mat.mtrl-sci

VO₂ (110)ᵣ 超薄膜中的电子相分离与非二聚化绝缘相的出现

Electronic phase separation and emergence of a nondimerized insulating phase in VO$_2$ $(110)_{\mathit{R}}$ ultrathin films

  • Tohoku University(东北大学)
  • High Energy Accelerator Research Organization (KEK)(高能加速器研究机构)
  • Université Paris-Saclay(巴黎-萨克雷大学)

机构由 AI 辅助整理,请以论文原文为准。

S. Inoue, D. Shiga, R. Hayasaka, K. Ozawa, A. F. Santander-Syro, H. Kumigashira

AI总结:

本研究通过原位光电子能谱和X射线吸收谱,发现VO₂ (110)ᵣ超薄膜中存在电子相分离,其非二聚化绝缘相比例随厚度减小呈指数增长,维度降低引发的莫特不稳定性是该相出现的关键驱动力。

AI中文摘要:

利用原位光电子能谱和X射线吸收谱,我们研究了VO₂/TiO₂ (110)超薄膜中电子结构与V-V二聚化的厚度依赖性,其中沿cᵣ轴的一维V-V链位于薄膜平面内。在VO₂ (110)ᵣ薄膜中,与VO₂ (001)ᵣ薄膜不同,沿表面法向的维度降低预计不会对V-V二聚化施加几何约束。然而,厚薄膜中观测到的与温度驱动金属-绝缘体转变相关的特征光谱变化持续到1.5 nm,而在1 nm时观测到无V-V二聚化的绝缘电子相。该行为与VO₂ (001)ᵣ的报道高度相似,表明维度降低导致的莫特不稳定性增强是VO₂超薄膜中非二聚化绝缘相出现的共同且必要驱动力。同时,与VO₂ (001)ᵣ不同,VO₂ (110)ᵣ中的非二聚化绝缘相与表现出温度驱动金属-绝缘体转变的相共存,其比例随厚度减小呈指数增长,在1 nm时成为主导相,对应的有效临界厚度估计为2.2 nm。这些结果表明,V-V链的几何取向通过应变介导的相竞争决定了电子相分离的空间演化。

英文摘要:

Using in situ photoemission spectroscopy and x-ray absorption spectroscopy, we investigated the thickness dependence of the electronic structure and V-V dimerization in VO$_2$/TiO$_2$ (110) ultrathin films, in which the one-dimensional V-V chains along the $c_{\mathit{R}}$ axis lie in the film plane. In VO$_2$ $(110)_{\mathit{R}}$ films, the reduction in dimensionality along the surface-normal direction is not expected to impose a geometric constraint on V-V dimerization, unlike in VO$_2$ $(001)_{\mathit{R}}$ films. Nevertheless, the characteristic spectral changes associated with the temperature-driven metal-insulator transition observed in thick films persist down to 1.5 nm, whereas at 1 nm an insulating electronic phase is observed without V-V dimerization. This behavior is highly similar to that reported for VO$_2$ $(001)_{\mathit{R}}$, suggesting that the enhancement of Mott instability resulting from reduced dimensionality is a common and essential driving force for the emergence of the nondimerized insulating phase in VO$_2$ ultrathin films. Meanwhile, unlike in VO$_2$ $(001)_{\mathit{R}}$, the nondimerized insulating phase in VO$_2$ $(110)_{\mathit{R}}$ coexists with the phase exhibiting the temperature-driven metal-insulator transition. Its fraction increases exponentially with decreasing thickness and becomes dominant at 1 nm. The corresponding effective critical thickness is estimated to be 2.2 nm. These results imply that the geometric orientation of the V-V chains dictates the spatial evolution of electronic phase separation via strain-mediated phase competition.

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