Apr 24, 2024
5:00pm - 7:00pm
Flex Hall C, Level 2, Summit
You Seung Rim1,Jiyoung Min1,Madani Labed1,Hyungseok Kim2,Kyungwho Choi3,Teakjib Choi1
Sejong University1,Korea Institute of Science and Technology2,Sungkyunkwan University3
Recently, beta gallium oxide (β-Ga
2O
3, 4.7–4.9eV), which has a wide band gap than SiC and GaN, has been attracting attentions in the field of power electronic applications [1]. The Baliga’s figure of merit(B-FOM) of Ga
2O
3 is about 3000, which is 4 times that of GaN and 10 times that of SiC, and is expected to achieving high breakdown voltage at low on-resistance in the power device [2]. However, despite these high numbers, the actual reported performance of the power unit is much lower than expected. This is because it is difficult to implement p-type Ga
2O
3, which can be used as PN junction termination to improve breakdown voltage value [3]. For further improvement of devices which require lower on-resistance(R
on) and higher breakdown voltage, it is important to form a junction termination structure such as a guard ring and a merged structure using a p-type material even to reduce the maximum electric field of a wide bandgap materials. However, the development of p-type β-Ga
2O
3 remains insufficient, only the theoretical studies and few experimental results reported. Because a very low mobility of self-trap holes and a deep acceptor level are expected, p-type β-Ga
2O
3 may intrinsically not be practical for power device applications. As a strategy to compensate for this is to construct p–n heterojunctions by integrating n-type Ga
2O
3 with other p-type semiconductors if the interface quality is controlled in an appropriate manner [4].
In this study, a diode to form a p-n heterojunction with optimized β-Ga
2O
3 was fabricated using NiO, a material with p-type conductivity [5]. Among p-type oxide families, the wide-bandgap NiO material has promising potentials in the applications of various optoelectronic and power devices due to its high visible spectral transparency and p-type conductivity stemming from nickel vacancies or monovalent impurities [6].
It was confirmed that the p-type NiO was inserted between the β-Ga
2O
3 and the Ni Schottky junction to ensure the p-n characteristics and thus the depletion layer expanded. In addition, the conductivity control of nickel oxide was attempted by lithium doping and oxygen concentration regulation. As a result, lithium-doped nickel oxide exhibited improved ohmic contact properties with Ni due to the thin film's low specific resistance characteristics compared to undoped nickel oxide, which induced the diode's low on-resistance. Therefore, using these current characteristics, NiO was stacked in two layers to design a heterojunction diode with a Li-NiO/NiO/β-Ga
2O
3 structure and a device that achieves a high breakdown voltage of -1678 V while maintaining a low on-resistance of 7.1 mΩcm
2Acknowledgments This work was supported by Korea Institute for Advancement of Technology (KIAT) grant funded by the Ministry of Trade, Industry & Energy (MOTIE, Korea) (P0012451, The Competency Development Program for Industry Specialist), the Technology Innovation Program - (20016102, Development of 1.2kV Gallium oxide power semiconductor devices technology and RS-2022-00144027, Development of 1.2kV-class low-loss gallium oxide transistor) funded by MOTIE, and Hyundai Motor Group.
References [1] M. Higashiwaki and G. H. Jessen, Appl. Phys. Lett. 112, 060401 (2018) [2] S. J. Pearton, F. Ren, M. Tadjer, and J. Kim, J. Appl. Phys. 124, 220901 (2018) [3] N. Allen, M. Xiao, X. D. Yan, IEEE Electron Device Lett. 40, 1399 (2019) [4] Y. Kokubun, S. Kubo, and S. Nakagomi, Appl. Phys. Express 9, 091101 (2016) [5] H. H. Gong, Appl. Phys. Lett. 117, 022104 (2020) [6] M. Tyagi, M. Tomar, V. Gupta, IEEE Electron Device Lett. 34, 81 (2013)