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Carrier Recombination Dynamics of Surface-Passivated Epitaxial (100)Ge, (110)Ge, and (111)Ge Layers by Atomic Layer Deposited Al2O3 Carrier Recombination Dynamics of Surface-Passivated Epitaxial (100)Ge, (110)Ge, and (111)Ge Layers by Atomic Layer Deposited Al2O3 AITranslate

Advanced Devices and Sustainable Energy Laboratory (ADSEL);National Renewable Energy Laboratory; CSIR-North East Institute of Science and Technology;Advanced Devices and Sustainable Energy Laboratory (ADSEL); Tezpur University; Tezpur University;Fluids Research Laboratory;Fluids Research Laboratory;Advanced Devices and Sustainable Energy Laboratory (ADSEL)
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Publisher: ACS
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Abstract AITranslate

Germanium (Ge) and its heterostructures with compound semiconductors offer a unique optoelectronic functionality due to its pseudo-bandgap nature, that can be transformed to a direct bandgap material by providing strain and/or mixing with tin. Moreover, two crystal surfaces, (100)Ge and (110)Ge, that are technologically important for ultralow power fin or nanosheet transistors, could offer unprecedented properties with reduced surface defects after passivating these surfaces by atomic layer deposited (ALD) dielectrics. In this work, the crystallographically oriented epitaxial Ge/AlAs heterostructures were grown and passivated with ALD Al2O3 dielectrics, and the microwave photoconductive decay (μ-PCD) technique was employed to evaluate carrier lifetimes at room temperature. The X-ray photoelectron spectroscopy analysis reveals no role of orientation effect in the quality of the ALD Al2O3 dielectric on oriented Ge layers. The carrier lifetimes measured using the μ-PCD technique were benchmarked against unpassivated Ge/AlAs heterostructures. Excitation wavelengths of 1500 and 1800 nm with an estimated injection level of ∼1013 cm–3 were selected to measure the orientation-specific carrier lifetimes. The carrier lifetime was increased from 390 ns to 565 ns for (100)Ge and from 260 ns to 440 ns for (110)Ge orientations with passivation, whereas the carrier lifetime is almost unchanged for (111)Ge after passivation. This behavior indicates a strong dependence of the measured lifetime on surface orientation and surface passivation. The observed increase (>1.5×) in lifetime with Al2O3-passivated (100)Ge and (110)Ge surfaces is due to the lower surface recombination velocity compared to unpassivated Ge/AlAs heterostructures. The enhancement of carrier lifetime from passivated Ge/AlAs heterostructures with (100)Ge and (110)Ge surface orientations offers a path for the development of nanoscale transistors due to the reduced interface state density.

KeyWords AITranslate

germanium Al2O3 molecular beam epitaxy Xray photoelectron spectroscopy lifetime atomic layer deposition
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DOI:https://doi.org/10.1021/acsaelm.3c00383

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Citation Information:

Germanium (Ge) and its heterostructures with compound semiconductors offer a unique optoelectronic functionality due to its pseudo-bandgap nature, that can be transformed to a direct bandgap material by providing strain and/or mixing with tin. Moreover, two crystal surfaces, (100)Ge and (110)Ge, that are technologically important for ultralow power fin or nanosheet transistors, could offer unprecedented properties with reduced surface defects after passivating these surfaces by atomic layer deposited (ALD) dielectrics. In this work, the crystallographically oriented epitaxial Ge/AlAs heterostructures were grown and passivated with ALD Al2O3 dielectrics, and the microwave photoconductive decay (μ-PCD) technique was employed to evaluate carrier lifetimes at room temperature. The X-ray photoelectron spectroscopy analysis reveals no role of orientation effect in the quality of the ALD Al2O3 dielectric on oriented Ge layers. The carrier lifetimes measured using the μ-PCD technique were benchmarked against unpassivated Ge/AlAs heterostructures. Excitation wavelengths of 1500 and 1800 nm with an estimated injection level of ∼1013 cm–3 were selected to measure the orientation-specific carrier lifetimes. The carrier lifetime was increased from 390 ns to 565 ns for (100)Ge and from 260 ns to 440 ns for (110)Ge orientations with passivation, whereas the carrier lifetime is almost unchanged for (111)Ge after passivation. This behavior indicates a strong dependence of the measured lifetime on surface orientation and surface passivation. The observed increase (>1.5×) in lifetime with Al2O3-passivated (100)Ge and (110)Ge surfaces is due to the lower surface recombination velocity compared to unpassivated Ge/AlAs heterostructures. The enhancement of carrier lifetime from passivated Ge/AlAs heterostructures with (100)Ge and (110)Ge surface orientations offers a path for the development of nanoscale transistors due to the reduced interface state density.

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GB/T 7714-2015 [1] Mantu K. Hudait, Steven W. Johnston, Manash R. Das, et al. ACS Applied Electronic Materials, 2023(5). DOI:10.1021/acsaelm.3c00383.
MLA [1] Mantu K. Hudait, et al., ACS Applied Electronic Materials, no. 5, 2023, https://doi.org/10.1021/acsaelm.3c00383.
APA [1] Mantu K. Hudait, Steven W. Johnston, Manash R. Das, Sengunthar Karthikeyan, Partha P. Sahu, Jagat Das, Jing Zhao, Robert J. Bodnar, & Rutwik Joshi. (2023). ACS Applied Electronic Materials(5). https://doi.org/10.1021/acsaelm.3c00383
IEEE [1] Mantu K. Hudait, Steven W. Johnston, Manash R. Das, Sengunthar Karthikeyan, Partha P. Sahu, Jagat Das, Jing Zhao, Robert J. Bodnar, and Rutwik Joshi, ACS Applied Electronic Materials, no. 5, 2023, doi: 10.1021/acsaelm.3c00383. keywords: {germanium Al2O3 molecular beam epitaxy Xray photoelectron spectroscopy lifetime atomic layer deposition}