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Incomplete Ionization of a 110 meV Unintentional Donor in β-Ga(2)O(3) and its Effect on Power Devices
Understanding the origin of unintentional doping in Ga(2)O(3) is key to increasing breakdown voltages of Ga(2)O(3) based power devices. Therefore, transport and capacitance spectroscopy studies have been performed to better understand the origin of unintentional doping in Ga(2)O(3). Previously unobs...
Autores principales: | , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
Nature Publishing Group UK
2017
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5643349/ https://www.ncbi.nlm.nih.gov/pubmed/29038456 http://dx.doi.org/10.1038/s41598-017-13656-x |
Sumario: | Understanding the origin of unintentional doping in Ga(2)O(3) is key to increasing breakdown voltages of Ga(2)O(3) based power devices. Therefore, transport and capacitance spectroscopy studies have been performed to better understand the origin of unintentional doping in Ga(2)O(3). Previously unobserved unintentional donors in commercially available [Formula: see text] Ga(2)O(3) substrates have been electrically characterized via temperature dependent Hall effect measurements up to 1000 K and found to have a donor energy of 110 meV. The existence of the unintentional donor is confirmed by temperature dependent admittance spectroscopy, with an activation energy of 131 meV determined via that technique, in agreement with Hall effect measurements. With the concentration of this donor determined to be in the mid to high 10(16) cm(−3) range, elimination of this donor from the drift layer of Ga(2)O(3) power electronics devices will be key to pushing the limits of device performance. Indeed, analytical assessment of the specific on-resistance (R(onsp)) and breakdown voltage of Schottky diodes containing the 110 meV donor indicates that incomplete ionization increases R(onsp) and decreases breakdown voltage as compared to Ga(2)O(3) Schottky diodes containing only the shallow donor. The reduced performance due to incomplete ionization occurs in addition to the usual tradeoff between R(onsp) and breakdown voltage. |
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