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High mobility Si(0.15)Ge(0.85) growth by using the molten target sputtering (MTS) within heteroepitaxy framework

High-speed SiGe film is promising use in photonics and electronics technologies continue to replace Si-based devices. High mobility Si(0.15) Ge(0.85) film on sapphire was grown at 890 °C substrate temperature by using a conventional magnetron sputtering system within the heteroepitaxy framework. 890...

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Detalles Bibliográficos
Autor principal: Kim, Hyun Jung
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group UK 2019
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6689090/
https://www.ncbi.nlm.nih.gov/pubmed/31399626
http://dx.doi.org/10.1038/s41598-019-47723-2
Descripción
Sumario:High-speed SiGe film is promising use in photonics and electronics technologies continue to replace Si-based devices. High mobility Si(0.15) Ge(0.85) film on sapphire was grown at 890 °C substrate temperature by using a conventional magnetron sputtering system within the heteroepitaxy framework. 890 °C substrate temperate is impractical for commercial device manufacturing due to long thermal soak, loading time, and costly process. To leverage the practical SiGe device applications, the Molten Target Sputtering (MTS) techniques is developed. The MTS is an economic and robust process from high flux density and liquid-state of molecules benefits. At 500 °C, the lowest substrate temperature, high mobility Si(0.15)Ge(0.85) film with continues morphology and 99.7% majority-orientation were grown by using the MTS. The hall electron mobilities of the Si(0.15)Ge(0.85) grown at 500 °C are 456 cm(2)V(−1)s(−1) and 123.9 cm(2)V(−1)s(−1) at 5.59 × 10(18) cm(3) and 3.5 × 10(20) cm(3) carrier concentration at 22.38 °C, respectively. The values are 550% higher hall electron mobilities than that of Si at equivalent carrier concentration and temperatures. We envision that the MTS is beneficial for the heteroepitaxy framework film growth that requires high substrate temperature to overcome the large lattice parameter mismatch between film and substrate.