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Thermionic Emission of Atomic Layer Deposited MoO(3)/Si UV Photodetectors

Ultrathin MoO(3) semiconductor nanostructures have garnered significant interest as a promising nanomaterial for transparent nano- and optoelectronics, owing to their exceptional reactivity. Due to the shortage of knowledge about the electronic and optoelectronic properties of MoO(3)/n-Si via an ALD...

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Detalles Bibliográficos
Autores principales: Basyooni, Mohamed A., Gaballah, A. E. H., Tihtih, Mohammed, Derkaoui, Issam, Zaki, Shrouk E., Eker, Yasin Ramazan, Ateş, Şule
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2023
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10095631/
https://www.ncbi.nlm.nih.gov/pubmed/37049060
http://dx.doi.org/10.3390/ma16072766
Descripción
Sumario:Ultrathin MoO(3) semiconductor nanostructures have garnered significant interest as a promising nanomaterial for transparent nano- and optoelectronics, owing to their exceptional reactivity. Due to the shortage of knowledge about the electronic and optoelectronic properties of MoO(3)/n-Si via an ALD system of few nanometers, we utilized the preparation of an ultrathin MoO(3) film at temperatures of 100, 150, 200, and 250 °C. The effect of the depositing temperatures on using bis(tbutylimido)bis(dimethylamino)molybdenum (VI) as a molybdenum source for highly stable UV photodetectors were reported. The ON–OFF and the photodetector dynamic behaviors of these samples under different applied voltages of 0, 0.5, 1, 2, 3, 4, and 5 V were collected. This study shows that the ultrasmooth and homogenous films of less than a 0.30 nm roughness deposited at 200 °C were used efficiently for high-performance UV photodetector behaviors with a high sheet carrier concentration of 7.6 × 10(10) cm(−2) and external quantum efficiency of 1.72 × 10(11). The electronic parameters were analyzed based on thermionic emission theory, where Cheung and Nord’s methods were utilized to determine the photodetector electronic parameters, such as the ideality factor (n), barrier height (Φ(0)), and series resistance (R(s)). The n-factor values were higher in the low voltage region of the I–V diagram, potentially due to series resistance causing a voltage drop across the interfacial thin film and charge accumulation at the interface states between the MoO(3) and Si surfaces.