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growth

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Book Chapter
Series: AIPP Books, Principles
Published: February 2023
10.1063/9780735425033_002
EISBN: 978-0-7354-2503-3
ISBN: 978-0-7354-2500-2
...Blevins, J. D. and Thomson, D., “β-Ga2O3 bulk growth techniques,” in Ultrawide Bandgap β-Ga2O3 Semiconductor: Theory and Applications, edited by J. S. Speck and E. Farzana (AIP Publishing, Melville, New York, 2023), pp. 2-1–2-26. In recent years, beta...
Book Chapter
Series: AIPP Books, Principles
Published: February 2023
10.1063/9780735425033_003
EISBN: 978-0-7354-2503-3
ISBN: 978-0-7354-2500-2
...Alema, F., Seryogin, G., and Osinsky, A., “MOCVD growth of β-Ga2O3 epitaxy,” in Ultrawide Bandgap β-Ga2O3 Semiconductor: Theory and Applications, edited by J. S. Speck and E. Farzana (AIP Publishing, Melville, New York, 2023), pp. 3-1–3-34...
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Nucleation and <span class="search-highlight">growth</span> of a stable nucleus which eventually evolves as a con...
Published: March 2023
FIG. 3.2 Nucleation and growth of a stable nucleus which eventually evolves as a continuous layer after having merged with other surviving nuclei. Nuclei (blue) having radii smaller than that of the critical nucleus disintegrate over time and therefore do not survive. More about this image found in Nucleation and growth of a stable nucleus which eventually evolves as a con...
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Schematic of the <span class="search-highlight">growth</span> configuration and the corresponding x-ray diffracti...
Published: March 2023
FIG. 7.6 Schematic of the growth configuration and the corresponding x-ray diffraction pattern of the BFO layers with constant thickness and LSMO with varying thicknesses [tetragonal (a), mixed (b), and rhombohedral (c)]. More about this image found in Schematic of the growth configuration and the corresponding x-ray diffracti...
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(a) Substrate and film with lattice parameters      a  s      and      a  0...
Published: March 2023
FIG. 3.13 (a) Substrate and film with lattice parameters a s and a 0 , respectively, where a s < a 0 . (b) Pseudomorphic growth with compressive strain. (c) Misfit dislocation of thin-film growth beyond critical thickness. More about this image found in (a) Substrate and film with lattice parameters a s and a 0...
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<span class="search-highlight">Growth</span> rate dependence on Ga flux for various <span class="search-highlight">growth</span> orientations.    Repro...
Published: February 2023
FIG. 4.2 Growth rate dependence on Ga flux for various growth orientations. Reproduced with permission from Oshima et al., Semicond. Sci. Technol. 33 (1), 015013 (2017). Copyright 2017 IOP Publishing. More about this image found in Growth rate dependence on Ga flux for various growth orientations. Repro...
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Maximum <span class="search-highlight">growth</span> rates vs <span class="search-highlight">growth</span> temperature across different orientations fo...
Published: February 2023
FIG. 4.3 Maximum growth rates vs growth temperature across different orientations for conventional PAMBE vs MOCATAXY (indium catalyzed growth). Reproduced with permission from Mauze et al., APL Mater. 8 (2), 021104 (2020b). Copyright 2020b AIP Publishing LLC. More about this image found in Maximum growth rates vs growth temperature across different orientations fo...
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Microstructural evolution in a thin film system with isotropic elasticity, ...
Published: March 2023
FIG. 8.6 Microstructural evolution in a thin film system with isotropic elasticity, the far-field composition is 0.05 leading to growth along with film break-up. From the top left, the microstructures correspond to (non-dimensional) time units: t = 114 600, t = 122 800, t = 133 800 and t = 205 800, respectively. These times indicate that the growth slows down the break-up dynamics compared to the previous case of (near) static break-up. More about this image found in Microstructural evolution in a thin film system with isotropic elasticity, ...
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Microstructural evolution in a thin film system with isotropic elasticity a...
Published: March 2023
FIG. 8.8 Microstructural evolution in a thin film system with isotropic elasticity and two films in the simulation cell, the far-field composition is 0.05 leading to growth along with film break-up. From top left, the microstructures correspond to (non-dimensional) time units: t = 110 800, t = 122 800, t = 143 400, and t = 270 800, respectively. These times indicate that the growth slows down the break-up dynamics compared to the previous case of (near) static break-up. More about this image found in Microstructural evolution in a thin film system with isotropic elasticity a...
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Diagram of oxygen delivery to a <span class="search-highlight">growth</span> furnace vs temperature for the growt...
Published: February 2023
FIG. 2.3 Diagram of oxygen delivery to a growth furnace vs temperature for the growth of large diameter β-Ga2O3 single crystals from an iridium crucible. RT—room temperature, TP—transition point, and MP—melting point ( Galazka et al., 2016 ). More about this image found in Diagram of oxygen delivery to a growth furnace vs temperature for the growt...
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<span class="search-highlight">Growth</span> rate vs TMGa molar flow rate for Ga<sub>2</sub>O<sub>3</sub> films g...
Published: February 2023
FIG. 3.8 Growth rate vs TMGa molar flow rate for Ga2O3 films grown using Agilis 500 and 700. Reprinted from Seryogin et al., Appl. Phys. Lett. 117 , 262101 (2020). Copyright 2020 AIP Publishing LLC. More about this image found in Growth rate vs TMGa molar flow rate for Ga2O3 films g...