2021
DOI: 10.1063/5.0052601
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Electron beam probing of non-equilibrium carrier dynamics in 18 MeV alpha particle- and 10 MeV proton-irradiated Si-doped β -Ga2O3 Schottky rectifiers

Abstract: Minority hole diffusion length and lifetime were measured in independent experiments by electron beam-induced current and time-resolved cathodoluminescence in Si-doped β-Ga2O3 Schottky rectifiers irradiated with 18 MeV alpha particles and 10 MeV protons. Both diffusion length and lifetime exhibited a decrease with increasing temperature. The non-equilibrium minority hole mobility was calculated from the independently measured diffusion length and lifetime, indicating that the so-called hole self-trapping is mo… Show more

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Cited by 14 publications
(17 citation statements)
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“…26,27,29,[45][46][47][48] The self-localization of excitons occurs at O(I) and O(II) site, corresponding to UVL ′ and UVL bands, respectively. 47,49 Although, as has been shown from Electron Paramagnetic Resonance (EPR) measurements 50 and confirmed by several independent EBIC studies on n-type β-Ga 2 O 3 , [20][21][22][23]39,51,52 the self-localization of holes is unstable above 110 K, the optical signature of the self-trapped excitons persists in CL and photoluminescence (PL) measurements. Note that the relative contribution of UVL ′ and UVL bands in both A and B samples is much lower than in n-type β-Ga 2 O 3 , found in earlier reports.…”
supporting
confidence: 54%
See 1 more Smart Citation
“…26,27,29,[45][46][47][48] The self-localization of excitons occurs at O(I) and O(II) site, corresponding to UVL ′ and UVL bands, respectively. 47,49 Although, as has been shown from Electron Paramagnetic Resonance (EPR) measurements 50 and confirmed by several independent EBIC studies on n-type β-Ga 2 O 3 , [20][21][22][23]39,51,52 the self-localization of holes is unstable above 110 K, the optical signature of the self-trapped excitons persists in CL and photoluminescence (PL) measurements. Note that the relative contribution of UVL ′ and UVL bands in both A and B samples is much lower than in n-type β-Ga 2 O 3 , found in earlier reports.…”
supporting
confidence: 54%
“…The incorporation of doped layers in devices such as Schottky diodes and field-effect transistors (FETs), including metal-oxide-semiconductor FETs (MOSFETs), and their ability to withstand high energy particle radiation have been explored. [15][16][17][18][19][20][21][22][23][24] Replicating these results to achieve p-type conductivity in β-Ga 2 O 3 has proven very difficult due to factors such as doping asymmetry, high compensation of acceptors, the high ionization energy of acceptor levels, and hole-trapping at O(I) and O(II) sites. [25][26][27][28][29][30] Despite these difficulties, native p-type conductivity was demonstrated at high temperatures in undoped β-Ga 2 O 3 .…”
mentioning
confidence: 99%
“…Efforts to address these issues have been underway over the past two decades. Substantial progress has also been made in designing radiation‐hard thin films transistors (TFTs) with ZnO, Ga 2 O 3 , In 2 O 3 , SnO 2 , IGZO, SiC, GaN, and many other WBGs, [ 17–50 ] which are used in the CMOS integrated circuits (ICs) over a long period under various radiations. Emerging memory technologies were also developed to stabilize the data storage performance in high temperatures and extremely harsh environments.…”
Section: Introductionmentioning
confidence: 99%
“…The large, spherical nsorbitals in the conduction band (CB) of MOS also play a critical role in high dopability for hosting a high density of electrons, leading to the remarkably tolerance to various radiation fluences. [17][18][19][20][21][22][23][24][25][26][27][28][29][30][31][32][33][34][35] Understanding the apparent immunity of the WBGs to various radiation environments and radiation-hard electronic engineering would be critical for pushing the technology further and understanding its limitations. Efforts to address these issues have been underway over the past two decades.…”
mentioning
confidence: 99%
“…There are a few direct techniques for observing carrier dynamics. Electron beam-induced current (EBIC) is a technique used to determine the minority carrier diffusion length [27][28][29][30][31][32][33]. The pump-probe technique, which is a timeresolved method, has been applied to β-Ga 2 O 3 [34,35], and the hole self-trapping coefficient was estimated to be 6.4 × 10 −8 cm 3 s −1 [35].…”
Section: Introductionmentioning
confidence: 99%