2022
DOI: 10.1016/j.apsusc.2022.154440
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First demonstration of hetero-epitaxial ε-Ga2O3 MOSFETs by MOCVD and a F-plasma surface doping

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Cited by 17 publications
(7 citation statements)
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“…The peak with lower binding energy (O A ) should be related to lattice oxygen (O 2− ), and the peak with higher binding energy (O B ) corresponds to oxygen vacancies. 22,46,47 As we can see, the O B peak of pure ε-Ga 2 O 3 film is more pronounced, and tends to disappear after the introduction of Zn, indicating that the introduction of Zn inhibits the generation of oxygen vacancies.…”
Section: Resultsmentioning
confidence: 83%
See 1 more Smart Citation
“…The peak with lower binding energy (O A ) should be related to lattice oxygen (O 2− ), and the peak with higher binding energy (O B ) corresponds to oxygen vacancies. 22,46,47 As we can see, the O B peak of pure ε-Ga 2 O 3 film is more pronounced, and tends to disappear after the introduction of Zn, indicating that the introduction of Zn inhibits the generation of oxygen vacancies.…”
Section: Resultsmentioning
confidence: 83%
“…20,21 Compared to b-Ga 2 O 3 , e-Ga 2 O 3 has a similar wide bandgap (B4.9 eV), higher lattice symmetry, lower anisotropic crystal structure, and lower growth temperature. [22][23][24][25] In recent years, research studies on solar-blind UV detectors based on e-Ga 2 O 3 thin films have begun to rise and are receiving increasing attention. [26][27][28] Although many efforts are being dedicated towards developing high-performance e-Ga 2 O 3 thin film solar-blind detectors, it is still a big challenge to simultaneously achieve low dark current, high specific detectivity, high UVvisible rejection ratio and quick response speed.…”
Section: Introductionmentioning
confidence: 99%
“…The LFOMs of the OD and HSD devices are 2.4 and 7.8 MW/cm 2 , respectively. The electrical characteristics of the heteroepitaxial Ga 2 O 3 MOSFETs are summarized in Table 1 [ 18 , 38 , 39 , 40 , 41 , 42 ]. Some parameters are missing because they were not discussed in the published results.…”
Section: Resultsmentioning
confidence: 99%
“…Even though the bandgap of 𝜖-Ga 2 O 3 is lower than that of AlN, our previous work has shown that 𝜖-Ga 2 O 3 thin films grown by MOCVD possess a resistivity of ≈10 4 Ωcm, which is high enough for RF resonator application. [44] To date, for the fabrication of RF resonators, AlN thin film is usually grown by Magnetron Sputtering at low temperature, [30][31][32] which is much easier than the MOCVD growth of 𝜖-Ga 2 O 3 investigated in this work. However, 𝜖-Ga 2 O 3 has demonstrated such a unique property that it possesses a good balance between the bandgap (resistivity) and piezoelectricity and is a better material choice for application in RF resonators.…”
Section: Resultsmentioning
confidence: 99%