Session Index

Special Session. Ultrawide-bandgap materials and devices

Special Session. Ultrawide-bandgap materials and devices
Wednesday, Nov. 12, 2025  09:15-11:30
Presider: Prof. Hsin-Ying Lee (National Cheng Kung University, Taiwan) Prof. Sheng-Po Chang (National Kaohsiung University of Science and Technology, Taiwan)
Room: 2nd Lecture Room
09:15 - 09:45
Manuscript ID.  0136
Paper No.  2025-Wed-S1105-I001
Invited Speaker:
Prof. Masataka Higashiwaki
Nitrogen doping technology for Ga2O3 devices

Prof. Masataka Higashiwaki, Professor, Osaka Metropolitan University, Japan

Nitrogen (N) atoms doped in gallium oxide (Ga2O3) act as deep acceptors, and an energy barrier of about 3 eV can be formed at the N-doped p-Ga2O3/n-Ga2O3 junction. In this talk, we will present the effect of N radical irradiation on electrical properties of Ga2O3 Schottky barrier diodes and electrical properties of N-doped Ga2O3 thin films grown by molecular beam epitaxy.

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09:45 - 10:15
Manuscript ID.  0133
Paper No.  2025-Wed-S1105-I002
Invited Speaker:
Prof. Okhyun Nam
Recent Advances in Heteroepitaxial Diamond: From Single Crystal Substrate to Devices

Okhyun Nam, Tech University of Korea, South Korea

Diamond is an ultra-wide bandgap semiconductor material which has high critical electric field (10 MVcm-1), high carrier mobility (e:4500 cm2/Vs, h:3800 cm2/Vs), and excellent thermal conductivity (2200 Wm-1K-1). Therefore, the diamond-based power device is a next-generation promising semiconductor device platform that can be used in an extreme environment requiring ultra-high power and frequency performance. The most important issue to solve for commercialization is the small size and too high price of diamond.
In our study, the activities for the growth of large size single crystal diamond substrate have been conducting using the heteroepitaxy on the foreign substrate. In case of (100) plane, we achieved the heteroepitaxy of free-standing single crystal diamond wafer (size: 20x20 mm2) on the A-plane sapphire substrate in the last year [1-2], and are working on the heteroepitaxy of larger-size diamond wafer (>1inch).[3] Especially, the twin-free (111) single crystal diamond heteroepitaxy has been successfully demonstrated on the r-plane sapphire substrate, for the first time.[3]
In addition, the heteroepitaxial single crystal diamond-based device study has been successfully conducted in the area of doping and devices of p-SBDs and p-MESFETs [4-5].
Recently, the H-terminated diamond E-/D-mode MOSFETs have been simultaneously fabricated on the same heteroepitaxial diamond substrate [6].
The detailed advancements in the heteroepitaxial diamond wafer and power devices will be discussed in the conference.


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10:15 - 10:30
Manuscript ID.  0032
Paper No.  2025-Wed-S1105-O001
Po-Kai Kung Phase Transformation and Ferroelectricity of ε(κ)-Ga2O3

Po-Kai Kung, Dong-Sing Wuu, Department of Applied Materials and Optoelectronic Engineering, National Chi Nan University, Nantou 54561, Taiwan; Wen-Hao Lee, Department of Materials Science and Engineering, National Chung Hsing University, Taichung 40227, Taiwan; Tung-Han Wu, Po-Liang Liu, Graduate Institute of Precision Engineering, National Chung Hsing University, Taichung 40227, Taiwan

Epsilon Gallium oxide (ε(κ)-Ga2O3), a ferroelectric wide-bandgap semiconductor, is heteroepitaxially grown on silicon using TiN buffer via MOCVD. The TiN buffer layer enables epitaxial growth with reduced lattice mismatch, resulting in a ε(κ)-Ga2O3 film with preferred orientation. The temperature is critical for phase transformation and crystallinity of ε(κ)-Ga2O3. The Ga2O3 progresses from amorphous phase to epsilon phase, ending up with beta phase as the temperature increases. Furthermore, the enhanced crystallinity leads to improved ferroelectricity, showing a polarizability of 0.04 µC/cm2. The optimized conditions yielded high-quality ε(κ)-Ga2O3 films (XRD FWHM 0.111°, ~3% oxygen vacancies) with uniformity across 2-inch wafers.

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10:30 - 10:45
Manuscript ID.  0063
Paper No.  2025-Wed-S1105-O002
Bernard Gil Effect of 2D carrier localization on light emission in (Al,Ga)N alloys emitting in the Deep UV range.

Alexandra Ibanez, Bernard Gil, Guillaume Cassabois, Pierre Valvin, Wilfried Desrat, UMR 5221, Laboratoire Charles Coulomb and Université Montpellier 2, Montpellier, 34095,France; Nikita Nikitskiy, Julien Brault, Mathieu Leroux, Antoine Barbier, Fabrice Semond, CNRS-CRHEA, Université Côte d’Azur, Valbonne, 06560, France; Muhammad Khan, Hideki Hirayama, Fumiya Chugenji, Taiga Kirihara, RIKEN Cluster for Pioneering Research (CPR), 2-1 Hirosawa, Wako, Saitama 351-0198, Japan

This work investigates the optical properties of (Al,Ga)N heterostructures emitting between 310nm and 209nm. Photoluminescence (PL) analyses were conducted on thick epilayers, single and multiple quantum wells. Full width at half maximum of the PL, orientations and shapes of the on-side emission diagram, and PL intensity were analyzed by taking into account valence band symmetry, Quantum Confined Stark Effect, and 2D carrier localization.
This work was supported by ANR funding GANEX (ANR-11-LABX-0014) and DOPALGAN .


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10:45 - 11:00
Manuscript ID.  0072
Paper No.  2025-Wed-S1105-O003
Andrew Allerman Ultra-Wide Bandgap AlGaN Polarization Doped PolFET Heterostructures for RF Transistors with a Contact Resistance less than 1 ohm.mm

Andrew Allerman, Andrew M. Armstrong, Brianna A. Klein, Sandia National Laboratories, Albuquerque, NM, USA, 87185; Seungheon Shin, Yinxuan Zhu, Jon Pratt, Davide Orlandini, Siddharth Rajan, Department of Electrical and Computer Engineering, The Ohio State University, Columbus, Ohio, USA

Ultra-wide bandgap AlGaN alloys are being investigated for the next generation of RF transistors due to their similar saturation velocity and high critical electric field, compared to GaN-based HEMT technology. However, the potential of AlGaN transistors has not been realized due to the difficulty in forming low-resistance contacts to the UWBG bandgap AlGaN alloys. We present a PolFET heterostructure that avoids the electron barrier due to the abrupt compositional change found in conventional HEMTs, allowing for lower contact resistance and enabling shielding of the charge in PolFET channel to achieve low sheet resistance and high mobility.

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11:00 - 11:15
Manuscript ID.  0039
Paper No.  2025-Wed-S1105-O004
Ting-Chun Chang Investigation of Ga2O3-based NO2 Gas Sensors with Roughened Seed Layer

Ting-Chun Chang, Tun-Hui Yang, Hsin-Ying Lee, Department of Photonics, National Cheng Kung University, Tainan 701, Taiwan, Republic of China; Mu-Ju Wu, Program on Key Materials, Academy of Innovative Semiconductor and Sustainable Manufacturing, National Cheng Kung University, Tainan 701, Taiwan, Republic of China; Ching-Ting Lee, Institute of Microelectronics, Department of Electrical Engineering, National Cheng Kung University, Tainan 701, Taiwan, Republic of China

This study aimed to enhance the sensing performance of nitrogen dioxide (NO2) gas sensors using gallium oxide (Ga2O3) nanorods grown on a roughened seed layer and forming more n-n homojunctions. The roughened seed layer was fabricated using a nanoimprint system with a grating period of 1000 nm. The response of the resulting NO2 gas sensor was significantly enhanced from 14.6 to 35.5 under a NO2 concentration of 10 ppm, and the optimal operating temperature was also decreased from 260 oC to 240 oC, indicating a substantial improvement in the sensing performance.

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11:15 - 11:30
Manuscript ID.  0058
Paper No.  2025-Wed-S1105-O005
Ravi Ranjan Kumar Low interface trap density of 4H-SiC MIS capacitor with a boron nitride PECVD layer

Ravi Ranjan Kumar, Promit Kumar Khan, Niall Tumilty, National Yang Ming Chiao Tung University

We report on the direct growth of hexagonal boron nitride (hBN) on 4H-SiC by plasma-enhanced chemical vapor deposition (PECVD). The hBN layer is evaluated within a metal-insulator-semiconductor capacitor (MISCAP). Leakage current is 2.6 µA/cm^2, remaining unchanged after both negative and positive bias stress tests at 8 V for 1650 s. Capacitance-voltage measurements demonstrate good capacitance modulation with minimal dispersion from quasistatic to 1 MHz. The interface state density (Dit) was evaluated using both the high-low and C–ψ(s) methods, yielding a Dit of 4×10^11 cm^-2 ·eV^-1 and 9×10^11 cm-2 ·eV^-1, respectively.

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