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Calculated formation energy diagrams for shallow <span class="search-highlight">donor</span> substitutional Ga-si...
Published: February 2023
FIG. 6.2 Calculated formation energy diagrams for shallow donor substitutional Ga-site donor dopants in β-Ga2O3 including the group IV elements C, Si, Ge, and Sn. The results are shown for both (a) Ga-rich/O-poor conditions and (b) O-rich/Ga-poor conditions. More about this image found in Calculated formation energy diagrams for shallow donor substitutional Ga-si...
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The deep <span class="search-highlight">donor</span> level <em>E<sub>d</sub></em><sub>2</sub> at ∼
Published: February 2023
FIG. 6.6 The deep donor level Ed2 at ∼EC–0.12 eV (a) increases with Si doping in β-Ga2O3 ( Ghadi et al., 2020a ) and (b) associated effect of Ed2 level with an estimated increase of on-resistance due to incomplete ionization during forward bias operation of β-Ga2O3 Schottky diodes ( Neal et al., 2017 ). More about this image found in The deep donor level Ed2 at ∼
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The calculated transition levels of several candidate <span class="search-highlight">donor</span> dopants in β-(A...
Published: February 2023
FIG. 6.17 The calculated transition levels of several candidate donor dopants in β-(AlxGa1–x)2O3 alloys shown as a function of Al content, as adapted with permission from (a) Varley et al., Appl. Phys. Lett. 116 , 172104 (2020). Copyright 2020 AIP Publishing LLC and (b) Mu et al., Phys. Rev. B 105 (2022). Copyright 2020 AIP Publishing LLC. The lines denote the ε(±) transition for C, Si, and Sn, and the ε(±) transition for Ge, Zr, Hf, and Ta dopants on the most favorable cation sites. The CBM energy (shaded green and yellow) is plotted with respect to the VBM energy of Ga2O3 for all compositions using the calculated energies from Peelaers et al. (2018) . The Al content at which a given dopant's defect level falls within the bandgap and thus the dopant is no longer expected to efficiently ionize at room temperature is included in parentheses. More about this image found in The calculated transition levels of several candidate donor dopants in β-(A...
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Schematic diagram of the behavior of dopants or impurities that act as (a) ...
Published: February 2023
FIG. 6.1 Schematic diagram of the behavior of dopants or impurities that act as (a) shallow donors, (b) shallow acceptors, or (c) introduce deep levels that may change occupancy depending on the position of the Fermi level (εF). Ga2O3 has been shown to exhibit a number of shallow donor candidates as in (a) and deep levels as in (c) that may act as donors and/or acceptors, but no shallow acceptors as in (b) due to fundamental limitations of the electronic structure. More about this image found in Schematic diagram of the behavior of dopants or impurities that act as (a) ...
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Silicon dopant energy level detected from (a) temperature-dependent Hall co...
Published: February 2023
FIG. 6.5 Silicon dopant energy level detected from (a) temperature-dependent Hall concentration fitted with two-donor model showing a shallow donor level at 40 meV and deep donor level at 150 meV ( Feng et al., 2020 ). (b) The secondary level was also observed from admittance spectroscopy (capacitance–frequency at different temperatures). The arrow indicates the presence of inflection point in the Cf plot associated with the deep trap emission that causes dispersion at higher frequencies ( Neal et al., 2017 ). More about this image found in Silicon dopant energy level detected from (a) temperature-dependent Hall co...
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Deep levels in Al<sub>x</sub>Ga<sub>1-x</sub>N as a function of Al composit...
Published: February 2023
FIG. 1.7 Deep levels in AlxGa1-xN as a function of Al composition showing shallow to deep level transition of donor levels as the material transforms from WBG GaN to UWBG AlxGa1-xN ( Kamyczek et al., 2012 ). More about this image found in Deep levels in AlxGa1-xN as a function of Al composit...
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Formation energy diagram for Mg dopants in β-Ga<sub>2</sub>O<sub>3</sub> sh...
Published: February 2023
FIG. 6.12 Formation energy diagram for Mg dopants in β-Ga2O3 shown for (a) Ga-rich (O-poor) and (b) O-rich (Ga-poor) conditions as adapted from Ritter et al., Appl. Phys. Lett. 113 (5), 052101 (2018). Copyright 2018 AIP Publishing LLC and Peelaers et al., APL Mater. 7 (2), 022519 (2019). Copyright 2019 AIP Publishing LLC. The figures also illustrate that moving the Fermi level away from the CBM with acceptor doping can also enhance the incorporation of donors such as deep donor IrGa impurities which were shown to be present in higher concentrations in Mg-doped single crystals ( Ritter et al., 2018 ). More about this image found in Formation energy diagram for Mg dopants in β-Ga2O3 sh...
Book Chapter
Series: AIPP Books, Methods
Published: March 2023
10.1063/9780735425743_003
EISBN: 978-0-7354-2574-3
ISBN: 978-0-7354-2572-9
... (σacceptor) and donor (σdonor) segments, as follows: (3.4) E HB ( σ , σ ′ ) = a eff c HB min { 0 ; min [ 0 , σ donor + σ HB ] max [ 0 ; σ acceptor − σ HB ] } where there are three adjustable parameters...
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Calculated formation energy diagrams for several transition-metal substitut...
Published: February 2023
FIG. 6.3 Calculated formation energy diagrams for several transition-metal substitutional Ga-site donor dopants in β-Ga2O3 shown for both Ga-rich/O-poor conditions (a) and O-rich/Ga-poor conditions (b). Reproduced with permission from Saleh et al., Semicond. Sci. Technol. 35 , 04LT01 (2020). Copyright 2020 AIP Publishing LLC. More about this image found in Calculated formation energy diagrams for several transition-metal substitut...
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Sn dopant level (a) detection from temperature-dependent Hall measurements ...
Published: February 2023
FIG. 6.8 Sn dopant level (a) detection from temperature-dependent Hall measurements showing the donor energy level at 77 meV ( Mauze et al., 2020 ) and (b) comparison of Sn and Si in terms of available free carrier from Hall measurements vs SIMS concentration showing a drop of carrier concentration from Sn at high doping levels ( Baldini et al., 2016 ). More about this image found in Sn dopant level (a) detection from temperature-dependent Hall measurements ...
Book Chapter
Series: AIPP Books, Principles
Published: February 2023
10.1063/9780735425033_006
EISBN: 978-0-7354-2503-3
ISBN: 978-0-7354-2500-2
... Publishing, Melville, New York, 2023), pp. 6-1–6-26. This chapter will discuss dopant species in β-Ga2O3, using both density functional theory (DFT) and experimental studies, in order to provide the reader a background of donors and acceptors that can be used to modulate fundamental...
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
... using trimethylgallium (TMGa) and triethylgallium (TEGa) precursors are presented. Transport properties of Si and Ge doped Ga2O3 films grown by MOCVD were analyzed to characterize the purity of the films, identify donor states, and determine donor and acceptor concentrations...
Book Chapter
Series: AIPP Books, Principles
Published: February 2023
0
EISBN: 978-0-7354-2503-3
ISBN: 978-0-7354-2500-2
... , C. A. , Halliburton , L. E. , and Giles , N. C. , “ Deep donor behavior of iron in β-Ga2O3 crystals: Establishing the Fe4 +/3 + level ,” J. Appl. Phys.   128 ( 14 ), 145704 ( 2020 ). 10.1063/5.0021756 Harris , J. S. , Baker , J. N. , Gaddy , B. E...
Book Chapter
Series: AIPP Books, Principles
Published: February 2023
10.1063/9780735425033_005
EISBN: 978-0-7354-2503-3
ISBN: 978-0-7354-2500-2
...-Ga2O3 has a large band gap (4.8 eV) and can also be easily n-type doped by shallow donors ( Ueda et al., 1997 ; Oshima et al., 2007 ; Higashiwaki et al., 2012 ; Hwang et al., 2014 ; and Konishi et al., 2017 ). It is imperative to have a thorough...
Book
Book Chapter
Series: AIPP Books, Principles
Published: February 2023
10.1063/9780735425033_001
EISBN: 978-0-7354-2503-3
ISBN: 978-0-7354-2500-2
... by compensating donors with acceptors, it is challenging to nearly match the acceptor and donor concentration; thus, this is not a viable path for high-performance power devices. Furthermore, a high acceptor density can compromise device performance by increasing the intrinsic specific on-resistance...
Book Chapter
Series: AIPP Books, Principles
Published: February 2023
10.1063/9780735425033_004
EISBN: 978-0-7354-2503-3
ISBN: 978-0-7354-2500-2
... doping is not realizable due to high acceptor ionization energies, high hole effective masses, and the likelihood of polaron formation if a hole is created ( Peelaers and Van de Walle, 2015 ). This limits doping to donor dopants for conductive n-type films and acceptor doping to achieve semi...
Book Chapter
Series: AIPP Books, Principles
Published: February 2023
10.1063/9780735425033_011
EISBN: 978-0-7354-2503-3
ISBN: 978-0-7354-2500-2
...–zd) ( Schubert, 1994 ), where N2D is the areal density of the dopant atoms in cm−2, zd represents the location of the delta sheet where z direction is aligned with the growth axis. In an ideal delta sheet, all the donors are located...
Book Chapter
Series: AIPP Books, Principles
Published: February 2023
0
EISBN: 978-0-7354-2503-3
ISBN: 978-0-7354-2500-2
... ( 2018 ). 10.1088/1361-6641/aaba98 Lyons , J. L. , Steiauf , D. , Janotti , A. , and Van De Walle , C. G. , “ Carbon as a shallow donor in transparent-conducting oxides ,” Phys. Rev. Appl.   2 , 064005 ( 2014 ). 10.1103/PhysRevApplied.2.064005 Ma , N. , Tanen , N...
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