Abstract
Amorphous gallium oxide thin films were grown by plasma-enhanced atomic layer deposition on (100) silicon substrates from trimethylgallium Ga(CH3)3 precursor and oxygen plasma. At 200 °C, the growth per cycle is in the range of 0.65–0.70 Å for O2 plasma exposure times ranging from 3 up to 30 s during each cycle. The effect of O2 plasma exposure times on the interfacial SiOx regrowth and the electrical properties was investigated. In situ spectroscopic ellipsometry shows that the SiOx regrowth occurs during the first three cycles and is limited to 0.27 nm for plasma times as long as 30 s. Increasing the O2 plasma exposure during each ALD cycle leads to a drastic decrease in the leakage current density (more than 5 orders of magnitude for 30 nm films), which is linked to the suppression of oxygen vacancy states as evidenced by spectroscopic ellipsometry. Interestingly, an increase in the dielectric constant with increasing O2 plasma exposure time is observed, reaching a value of εr∼14.2, larger than that of single crystalline β-Ga2O3. This study highlights the crucial role of oxygen plasma exposure time in the control and tuning of the electrical properties of amorphous gallium oxide films.
Highlights
Ga2O3 crystallizes in five different polymorphs, among which the monoclinic β-phase is the stable phase at room temperature and atmospheric pressure.[1]
Amorphous gallium oxide thin films were grown by plasma-enhanced atomic layer deposition on (100) silicon substrates from trimethylgallium Ga(CH3)[3] precursor and oxygen plasma
We focus on the effect of O2 plasma exposure time on the dielectric permittivity and leakage current density JL of amorphous gallium oxide films deposited by plasma-enhanced atomic layer deposition (ALD)
Summary
Ga2O3 crystallizes in five different polymorphs, among which the monoclinic β-phase is the stable phase at room temperature and atmospheric pressure.[1]. Thin amorphous GaOx layers have been shown to be an effective electron transport layer in CIGS- or CuO2-based solar cells,[13,14] to act as an effective passivation layer for c-Si solar cells,[15] and to be an effective tunneling barrier to reduce electron recombination in dye-sensitized solar cells.[16]
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More From: Journal of Vacuum Science & Technology A: Vacuum, Surfaces, and Films
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