(Invited) Radiation Damage in the Ultra Wide Bandgap Semiconductor Ga 2 O 3

Ga 2 O 3 is expected to show similar radiation resistance as GaN and SiC, considering their average bond strengths. However, this is not enough to explain the orders of magnitude difference of the relative resistance to radiation damage of these materials compared to GaAs and dynamic annealing of de...

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Veröffentlicht in:ECS transactions 2022-09, Vol.109 (3), p.165-187
Hauptverfasser: Xia, Xinyi, Li, Jian-Sian, Sharma, Ribhu, Ren, Fan, Rasel, Md Abu Jafar, Stepanoff, Sergei, Al-Mamun, Nahid, Haque, Amanul, Wolfe, Douglas, Modak, Sushrut, Chernyak, Leonid, Law, Mark, Khachatrian, Ani, Pearton, Stephen J
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container_issue 3
container_start_page 165
container_title ECS transactions
container_volume 109
creator Xia, Xinyi
Li, Jian-Sian
Sharma, Ribhu
Ren, Fan
Rasel, Md Abu Jafar
Stepanoff, Sergei
Al-Mamun, Nahid
Haque, Amanul
Wolfe, Douglas
Modak, Sushrut
Chernyak, Leonid
Law, Mark
Khachatrian, Ani
Pearton, Stephen J
description Ga 2 O 3 is expected to show similar radiation resistance as GaN and SiC, considering their average bond strengths. However, this is not enough to explain the orders of magnitude difference of the relative resistance to radiation damage of these materials compared to GaAs and dynamic annealing of defects is much more effective in Ga 2 O 3 . Octahedral gallium monovacancies are the main defects produced under most radiation conditions because of the larger cross-section for interaction compared to oxygen vacancies. Proton irradiation introduces two main paramagnetic defects in Ga 2 O 3 , which are stable at room temperature. Charge carrier removal can be explained by Fermi-level pinning far from the conduction band minimum due to gallium interstitials (Ga i ), vacancies (V Ga ), and antisites (Ga O ). With few experimental or simulation studies on single event effects (SEE) in Ga 2 O 3 , it is apparent that while other wide bandgap semiconductors like SiC and GaN are robust against displacement damage and total ionizing dose, they display significant vulnerability to single event effects at high Linear Energy Transfer (LET) and at much lower biases than expected. We have analyzed the transient response of β-Ga 2 O 3 rectifiers to heavy-ion strikes via TCAD simulations. Using field metal rings improves the breakdown voltage and biasing those rings can help control the breakdown voltage. Such biased rings help in the removal of the charge deposited by the ion strike.
doi_str_mv 10.1149/10903.0165ecst
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However, this is not enough to explain the orders of magnitude difference of the relative resistance to radiation damage of these materials compared to GaAs and dynamic annealing of defects is much more effective in Ga 2 O 3 . Octahedral gallium monovacancies are the main defects produced under most radiation conditions because of the larger cross-section for interaction compared to oxygen vacancies. Proton irradiation introduces two main paramagnetic defects in Ga 2 O 3 , which are stable at room temperature. Charge carrier removal can be explained by Fermi-level pinning far from the conduction band minimum due to gallium interstitials (Ga i ), vacancies (V Ga ), and antisites (Ga O ). With few experimental or simulation studies on single event effects (SEE) in Ga 2 O 3 , it is apparent that while other wide bandgap semiconductors like SiC and GaN are robust against displacement damage and total ionizing dose, they display significant vulnerability to single event effects at high Linear Energy Transfer (LET) and at much lower biases than expected. We have analyzed the transient response of β-Ga 2 O 3 rectifiers to heavy-ion strikes via TCAD simulations. Using field metal rings improves the breakdown voltage and biasing those rings can help control the breakdown voltage. 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title (Invited) Radiation Damage in the Ultra Wide Bandgap Semiconductor Ga 2 O 3
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