Huo Fangfang, Muydinov Ruslan, Seibertz Bertwin Bilgrim Otto, Wang Can, Hartig Manuel, Alktash Nivin, Gao Peng, Szyszka Bernd
Institute für High-Frequency and Semiconductor-System Technologies, Technische Universität Berlin, Einsteinufer 25, 10587, Berlin, Germany.
CAS Key Laboratory of Design and Assembly of Functional Nanostructures, and Fujian Provincial Key Laboratory of Nanomaterials Fujian Institute of Research on the Structure of Matter, Chinese Academy of Sciences, 350002, Fuzhou, Fujian, China.
Heliyon. 2024 May 10;10(10):e30943. doi: 10.1016/j.heliyon.2024.e30943. eCollection 2024 May 30.
SnO and tantalum doped SnO (TTO) thin films were prepared using reactive hollow cathode gas flow sputtering (GFS) on glass substrates. An in-situ heating process under vacuum preceded the sputtering. The resistivity of the tin oxide films was reduced to a remarkable low of 2.02 × 10 Ω cm, with a carrier concentration of 2.55 × 10 cm and a mobility of 12.11 cmVs. As the substrate temperature increased, the film resistivity decreased. Notably, at a substrate temperature of 270 °C, the effect of Ta doping on the film resistivity and carrier concentration was significantly stronger compared to higher temperatures. Elevating the substrate temperature and Ta doping resulted in a lower refractive index (n). This effect was consistently strong at higher temperatures, attributed to the higher film-free carrier concentration (4.54 × 10 cm) compared to lower temperatures (2.35 × 10 cm). The film's structure was characterized by scanning electron microscopy (SEM), X-ray diffraction (XRD) and atomic force microscope (AFM). The preferred direction of film growth was discussed. The successful and reproducible fabrication of tin oxide films underscores the advantages of gas flow sputtering (GFS) technology. GFS offers stable operating conditions across various oxygen flow levels without requiring target oxidization control, as is required in magnetron sputtering when managing gas status and film quality.
采用反应性空心阴极气体流动溅射(GFS)在玻璃衬底上制备了SnO和钽掺杂的SnO(TTO)薄膜。溅射之前在真空下进行原位加热过程。氧化锡薄膜的电阻率显著降低至2.02×10Ω·cm的低值,载流子浓度为2.55×10cm,迁移率为12.11cm²V⁻¹s⁻¹。随着衬底温度升高,薄膜电阻率降低。值得注意的是,在270°C的衬底温度下,与更高温度相比,Ta掺杂对薄膜电阻率和载流子浓度的影响明显更强。提高衬底温度和Ta掺杂会导致折射率(n)降低。在较高温度下这种影响一直很强,这归因于与较低温度(2.35×10cm)相比更高的薄膜自由载流子浓度(4.54×10cm)。通过扫描电子显微镜(SEM)、X射线衍射(XRD)和原子力显微镜(AFM)对薄膜结构进行了表征。讨论了薄膜生长的择优方向。氧化锡薄膜的成功且可重复制备突出了气体流动溅射(GFS)技术的优势。GFS在各种氧气流量水平下都提供稳定的操作条件,无需像磁控溅射在管理气体状态和薄膜质量时那样进行靶材氧化控制。