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Deep-UV Transparent Conducting Oxide La-Doped SrSnO(3) with a High Figure of Merit

[Image: see text] Perovskite stannate SrSnO(3) (SSO) is attracting attention as ultraviolet transparent conducting oxides (UV TCOs) due to its ultrawide band gap and high conductivity. Here, we investigate in detail the thickness-dependent electrical, structural, and optical properties of sequential...

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Detalles Bibliográficos
Autores principales: Kim, Juhan, Yun, Hwanhui, Seo, Jihoon, Kim, Jae Ha, Kim, Jae Hoon, Mkhoyan, K. Andre, Kim, Bongju, Char, Kookrin
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Chemical Society 2022
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9344396/
https://www.ncbi.nlm.nih.gov/pubmed/35937184
http://dx.doi.org/10.1021/acsaelm.2c00581
Descripción
Sumario:[Image: see text] Perovskite stannate SrSnO(3) (SSO) is attracting attention as ultraviolet transparent conducting oxides (UV TCOs) due to its ultrawide band gap and high conductivity. Here, we investigate in detail the thickness-dependent electrical, structural, and optical properties of sequentially strain-relaxed La-doped SrSnO(3) (SLSO) epitaxial thin films. We find that the SLSO films grow as an orthorhombic Pnma phase with a(–)a(–)c(+) in the c(+) direction under the tensile strain. With the strain relaxation, as the films become thicker, vertical grain boundaries are created and the orthorhombic phase becomes reoriented to all three possible orientations. Simultaneously, the conductance starts to deviate from the linear behavior with increasing film thickness. Through the analysis of thickness fringes in optical transmittance, we found that a 120 nm thick nominally 4% La-doped SrSnO(3) film has a figure of merit (φ(TC) = 2.65 × 10(–3) Ω(–1)) at λ = 300 nm in the deep-UV region, which is the highest value among the well-known candidates for UV TCOs reported to date.