578 research outputs found

    The 2018 GaN Power Electronics Roadmap

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    Gallium nitride (GaN) is a compound semiconductor that has tremendous potential to facilitate economic growth in a semiconductor industry that is silicon-based and currently faced with diminishing returns of performance versus cost of investment. At a material level, its high electric field strength and electron mobility have already shown tremendous potential for high frequency communications and photonic applications. Advances in growth on commercially viable large area substrates are now at the point where power conversion applications of GaN are at the cusp of commercialisation. The future for building on the work described here in ways driven by specific challenges emerging from entirely new markets and applications is very exciting. This collection of GaN technology developments is therefore not itself a road map but a valuable collection of global state-of-the-art GaN research that will inform the next phase of the technology as market driven requirements evolve. First generation production devices are igniting large new markets and applications that can only be achieved using the advantages of higher speed, low specific resistivity and low saturation switching transistors. Major investments are being made by industrial companies in a wide variety of markets exploring the use of the technology in new circuit topologies, packaging solutions and system architectures that are required to achieve and optimise the system advantages offered by GaN transistors. It is this momentum that will drive priorities for the next stages of device research gathered here

    AlGaN/GaN ์ „๋ ฅ์†Œ์ž์˜ ํŠน์„ฑ ํ–ฅ์ƒ์„ ์œ„ํ•œ ์‹๊ฐ๊ณผ ์ ˆ์—ฐ๋ง‰์— ๊ด€ํ•œ ์—ฐ๊ตฌ

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    ํ•™์œ„๋…ผ๋ฌธ (๋ฐ•์‚ฌ) -- ์„œ์šธ๋Œ€ํ•™๊ต ๋Œ€ํ•™์› : ๊ณต๊ณผ๋Œ€ํ•™ ์ „๊ธฐยท์ •๋ณด๊ณตํ•™๋ถ€, 2020. 8. ์„œ๊ด‘์„.์ตœ๊ทผ ์—๋„ˆ์ง€ ์œ„๊ธฐ์™€ ํ™˜๊ฒฝ๊ทœ์ œ ๊ฐ•ํ™”, ์นœํ™˜๊ฒฝ ๋…น์ƒ‰์„ฑ์žฅ ๋“ฑ์˜ ์ด์Šˆ๊ฐ€ ๋Œ€๋‘๋˜์–ด ์—๋„ˆ์ง€ ์ ˆ๊ฐ๊ณผ ํ™˜๊ฒฝ ๋ณดํ˜ธ ๋ถ„์•ผ์— IT ๊ธฐ์ˆ ์„ ์ ‘๋ชฉ, ํ™œ์šฉํ•˜๋Š” ๊ทธ๋ฆฐ IT ํŒจ๋Ÿฌ๋‹ค์ž„์ด ๋ถ€๊ฐ๋˜๊ณ  ์žˆ๋‹ค. ํ˜„์žฌ ๊ณ ์œ ๊ฐ€ ํ™˜๊ฒฝ๊ทœ์ œ ๊ฐ•ํ™”์— ๋Œ€์‘ํ•˜๊ธฐ ์œ„ํ•ด ํ•˜์ด๋ธŒ๋ฆฌ๋“œ ์ž๋™์ฐจ, ์ „๊ธฐ์ž๋™์ฐจ ๋“ฑ ์นœํ™˜๊ฒฝ ๋ฏธ๋ž˜ํ˜• ์ž๋™์ฐจ ๊ฐœ๋ฐœ์ด ์š”๊ตฌ๋˜๊ณ  ์žˆ์œผ๋ฉฐ, ์ž๋™์ฐจ์—์„œ ์ „์žฅ๋ถ€ํ’ˆ์ด ์ฐจ์ง€ํ•˜๋Š” ์›๊ฐ€๋น„์ค‘์€ ์•ฝ 40%๊นŒ์ง€ ๋‹ฌํ•  ๊ฒƒ์œผ๋กœ ์ „๋ง๋˜๊ณ  ์ด ์ค‘ ๋ฐ˜๋„์ฒด๊ฐ€ ์ฐจ์ง€ํ•˜๋Š” ๋น„์šฉ์€ ์•ฝ 30% ์ •๋„๋กœ ์ถ”์ •๋œ๋‹ค. ์ด๋Ÿฌํ•œ ์ž๋™์ฐจ ์ „์žฅ๋ถ€ํ’ˆ์—์„œ ์ „๋ ฅ์†Œ์ž๊ฐ€ ํ•ต์‹ฌ๋ถ€ํ’ˆ์œผ๋กœ ์ž๋ฆฌ ์žก์„ ์ „๋ง์ด๋‹ค. ์ง€๊ธˆ๊นŒ์ง€๋Š” ์‹ค๋ฆฌ์ฝ˜ ๊ธฐ๋ฐ˜์˜ ์ „๋ ฅ์†Œ์ž ๊ธฐ์ˆ ์ด ์ „๋ ฅ๋ฐ˜๋„์ฒด ์‹œ์žฅ์˜ ๋Œ€๋ถ€๋ถ„์„ ์ฃผ๋„ํ•˜๊ณ  ์žˆ์ง€๋งŒ ์ „๋ ฅ๊ธฐ๊ธฐ ๋กœ๋“œ๋งต์— ์˜ํ•˜๋ฉด ์ „๋ ฅ๋ฐ€๋„๊ฐ€ ํ•ด๋ฅผ ๊ฑฐ๋“ญํ•˜๋ฉด์„œ ์ง€์†์ ์œผ๋กœ ์ฆ๊ฐ€ํ•˜๊ธฐ ๋•Œ๋ฌธ์— ๋‚ด์—ด, ๋‚ด์••, ์ „๋ ฅ์†์‹ค, ์ „๋ ฅ๋ฐ€๋„ ๋“ฑ์—์„œ ๋‚˜ํƒ€๋‚˜๋Š” ๋งŽ์€ ํ•œ๊ณ„๋ฅผ ๊ฐ€์ง€๊ณ  ์žˆ๋Š” ํ˜„์žฌ์˜ ์‹ค๋ฆฌ์ฝ˜ ๊ธฐ๋ฐ˜ ์ „๋ ฅ์‹œ์Šคํ…œ์€ ํšจ์œจ์ด ๋ˆˆ์— ๋„๊ฒŒ ๊ฐ์†Œํ•  ๊ฒƒ์ด ์ž๋ช…ํ•˜๋ฏ€๋กœ ์ „๋ ฅ์‹œ์Šคํ…œ์˜ ์ „๋ ฅ์ „์†กํšจ์œจ๊ณผ ์‹ ๋ขฐ์„ฑ์˜ ์ค‘์š”์„ฑ์ด ํฌ๊ฒŒ ๋Œ€๋‘๋˜๊ณ  ์žˆ๋‹ค. ์ด ๊ฐ™์€ ์‚ฌํšŒ์  ์š”๊ตฌ๋กœ ๋ณผ ๋•Œ ํ˜„์žฌ์˜ ์‹ค๋ฆฌ์ฝ˜ ์ „๋ ฅ์†Œ์ž์˜ ๊ธฐ์ˆ ์  ํ•œ๊ณ„๋ฅผ ๋›ฐ์–ด๋„˜๋Š” ๊ณ ํšจ์œจ์˜ ์ฐจ์„ธ๋Œ€ ์ „๋ ฅ๋ฐ˜๋„์ฒด ์†Œ์ž์˜ ๊ฐœ๋ฐœ์ด ์‹œ๊ธ‰ํžˆ ์š”๊ตฌ๋˜๋ฉฐ SiC์™€ GaN์™€ ๊ฐ™์€ ๊ด‘๋Œ€์—ญ ๋ฐ˜๋„์ฒด๊ฐ€ ์ฐจ์„ธ๋Œ€ ์ „๋ ฅ๋ฐ˜๋„์ฒด ์†Œ์žฌ๋กœ ์œ ๋ ฅํ•ด์ง€๊ณ  ์žˆ๋‹ค. ๋˜ํ•œ ์ „๋ ฅ์‹œ์Šคํ…œ์—์„œ๋Š” ์‹œ์Šคํ…œ์˜ ์•ˆ์ „์„ฑ๊ณผ ํšŒ๋กœ์˜ ๊ฐ„๋žตํ™”๋ฅผ ์œ„ํ•˜์—ฌ normally-off (์ฆ๊ฐ•ํ˜•) ์ „๋ ฅ์†Œ์ž๊ฐ€ ์š”๊ตฌ๋˜๊ธฐ ๋•Œ๋ฌธ์— normally-off (์ฆ๊ฐ•ํ˜•) GaN ์ „๋ ฅ์†Œ์ž์— ๋Œ€ํ•œ ๊ฐœ๋ฐœ์ด ํ•„์ˆ˜์ ์ด๋‹ค. ๋ณธ ๊ทธ๋ฃน์—์„œ๋Š” gate-recess ๊ณต์ •์„ ์ด์šฉํ•˜์—ฌ normally-off ๋™์ž‘์„ ์‹คํ˜„ํ•˜๋Š” ์—ฐ๊ตฌ๋ฅผ ์ง„ํ–‰ํ•˜์˜€๊ณ , gate-recess ์‹œ ๋ฐœ์ƒํ•˜๋Š” ์‹๊ฐ ๋ฐ๋ฏธ์ง€๋ฅผ ์ค„์ด๊ณ  ์šฐ์ˆ˜ํ•œ ์„ฑ๋Šฅ์˜ ๊ฒŒ์ดํŠธ ์ ˆ์—ฐ๋ง‰์„ ๊ฐœ๋ฐœํ•˜์—ฌ GaN ์ „๋ ฅ ๋ฐ˜๋„์ฒด ์†Œ์ž์˜ ์ „๊ธฐ์  ํŠน์„ฑ ๋ฐ ์‹ ๋ขฐ์„ฑ์„ ๊ฐœ์„ ํ•˜๋Š” ์—ฐ๊ตฌ๋ฅผ ์ง„ํ–‰ํ•˜์˜€๋‹ค. ์‹๊ฐ ์—ฐ๊ตฌ์—์„œ๋Š” ์ตœ์ข…์ ์œผ๋กœ ์…€ํ”„ DC ๋ฐ”์ด์–ด์Šค๊ฐ€ ๋‚ฎ์€ O2, BCl3 ํ”Œ๋ผ์ฆˆ๋งˆ๋ฅผ ์ด์šฉํ•œ atomic layer etching์„ ๊ฐœ๋ฐœํ•˜์˜€๊ณ , ์ด๋ฅผ ํ†ตํ•ด ๊ฑฐ์น ๊ธฐ๊ฐ€ ์ž‘๊ณ  ํ‘œ๋ฉด N vacancy๊ฐ€ ์ ์€ ๊ณ ํ’ˆ์งˆ์˜ (Al)GaN ํ‘œ๋ฉด์„ ์–ป์„ ์ˆ˜ ์žˆ์—ˆ๋‹ค. ๋ฐ•๋ง‰ ์—ฐ๊ตฌ์—์„œ๋Š” Oxide ๋ฐ•๋ง‰ ์ฆ์ฐฉ ์‹œ, (Al)GaN ํ‘œ๋ฉด์— ์ƒ์„ฑ๋˜์–ด ๊ณ„๋ฉด ํŠน์„ฑ์„ ์•…ํ™”์‹œํ‚ค๋Š” Ga2O3 ์ƒ์„ฑ์„ ๋ง‰๊ธฐ์œ„ํ•ด ALD AlN layer๋ฅผ ๊ฐœ๋ฐœ ๋ฐ ์ ์šฉํ•˜์—ฌ ๋ฐ•๋ง‰/(Al)GaN ๊ณ„๋ฉด ํŠน์„ฑ์„ ํ–ฅ์ƒ์‹œ์ผฐ๋‹ค. ์ด๋กœ ์ธํ•ด ์†Œ์ž์˜ ๋™์ž‘์ „๋ฅ˜ ์ฆ๊ฐ€ ๋ฐ Dit ๊ฐ์†Œ ๊ฒฐ๊ณผ๋ฅผ ์–ป์„ ์ˆ˜ ์žˆ์—ˆ๊ณ  ์ŠคํŠธ๋ ˆ์Šค์— ๋”ฐ๋ฅธ ๋ฌธํ„ฑ์ „์•• ์ด๋™ ํŠน์„ฑ์˜ ๊ฐ์†Œ๋กœ ์†Œ์ž์˜ ์‹ ๋ขฐ์„ฑ ๋˜ํ•œ ๊ฐœ์„ ์‹œํ‚ฌ ์ˆ˜ ์žˆ์—ˆ๋‹ค. ์ด๋Š” ํƒ€ ๊ธฐ๊ด€์˜ ๊ฒฐ๊ณผ์™€ ๋น„๊ตํ•ด๋„ ๋’ค๋–จ์–ด์ง€์ง€ ์•Š๋Š” ์šฐ์ˆ˜ํ•œ ํŠน์„ฑ์„ ๋ณด์—ฌ์ฃผ์—ˆ๋‹ค. ๊ฒฐ๋ก ์ ์œผ๋กœ ๋ณธ ์—ฐ๊ตฌ์˜ ์ž‘์€ ํ”Œ๋ผ์ฆˆ๋งˆ ๋ฐ๋ฏธ์ง€๋ฅผ ๊ฐ–๋Š” ์‹๊ฐ๊ณต์ •๊ณผ ๊ณ ํ’ˆ์งˆ ์ ˆ์—ฐ๋ง‰ ๊ฐœ๋ฐœ์„ ํ†ตํ•ด ์šฐ์ˆ˜ํ•œ ํŠน์„ฑ์˜ GaN ์ „๋ ฅ์†Œ์ž๋ฅผ ๊ตฌํ˜„ํ•  ์ˆ˜ ์žˆ์—ˆ๊ณ  ํ–ฅํ›„ ์ฐจ์„ธ๋Œ€ ์ „๋ ฅ์†Œ์ž์— ์ ์šฉ์„ ์œ„ํ•œ ๊ฐ€๋Šฅ์„ฑ์„ ํ™•๋ณดํ•˜์˜€๋‹ค.The Si technology for power devices have already approached its theoretical limitations due to its physical and material properties, despite the considerable efforts such as super junction MOSFET, trench gate, and insulated gate bipolar transistors. To overcome these limitations, many kinds of compound materials such as GaN, GaAs, SiC, Diamond and InP which have larger breakdown voltage and high electron velocity than Si also have been studied as future power devices. GaN has been considered as a breakthrough in power applications due to its high critical electric field, high saturation velocity and high electron mobility compared to Si, GaAs, and SiC. Especially, AlGaN/GaN heterostructure field-effect transistors (HFETs) have been considered as promising candidates for high power and high voltage applications. However, these AlGaN/GaN heterostructure field-effect transistors with the 2DEG are naturally normally-on, which makes the devices difficult to deplete the channel at zero gate bias. Among the various methods for normally-off operation of GaN devices, gate-recess method is a promising method because it can be easier to implement than other approaches and ensure normally-off operation. However, charge trapping at the interface between gate dielectric and (Al)GaN and in the gate dielectric is a big issue for recessed gate MIS-HEMTs. This problem leads to degradation of channel mobility, on-resistance and on-current of the devices. Especially, Vth hysteresis after a positive gate voltage sweep and Vth shift under a gate bias stress are important reliability challenges in gate recessed MIS-HEMTs. The scope of this work is mainly oriented to achieve high quality interface at dielectric/(Al)GaN MIS by studying low damage etching methods and the ALD process of various dielectric layers. In the etching study, various etching methods for normally-off operation have been studied. Also, etching damage was evaluated by various methods such as atomic force microscopy (AFM), photoluminescence (PL) measurements, X-ray photoelectron spectroscopy (XPS) measurements and electrical properties of the recessed schottky devices. Among the etching methods, the ALE shows the smoothest etched surface, the highest PL intensity and N/(Al+Ga) ratio of the etched AlGaN surface and the lowest leakage current of the gate recessed schottky devices. It is suggested that the ALE is a promising etching technique for normally-off gate recessed AlGaN/GaN MIS-FETs. In the study of dielectrics, excellent electrical characteristics and small threshold voltยฌage drift under positive gate bias stress are achieved by employing the SiON interfacial layer. However, considerable threshold voltage drift is observed under the higher positive gate bias stress even at the devices using the SiON interfacial layer. For further improvement of interface and reliability of devices, we develop and optimize an ALD AlN as an interfacial layer to avoid the formation of poor-quality oxide at the dielectric/(Al)GaN interface. We also develop an ALD AlHfON as a bulk layer, which have a high dielectric constant and low leakage current and high breakdown field characteristics. Devices with AlN/AlON/AlHfON layer show smaller I-V hysteresis of ~10 mV than that of devices with AlON/AlHfON layer. The extracted static Ron values of devices with AlN/AlON/AlHfON and AlON/AlHfON are 1.35 and 1.69 mโ„ฆยทcm2, respectively. Besides, the effective mobility, Dit and threshold voltage instability characteristics are all improved by employing the ALD AlN. In conclusion, for high performance and improvement of reliability of normally-off AlGaN/GaN MIS-FETs, this thesis presents an etching technique for low damage etching and high-quality gate dielectric layer and suggests that the ALE and ALD AlN/AlON/AlHfON gate dielectric are very promising for the future normally-off AlGaN/GaN MIS-FETsChapter 1. Introduction 1 1.1. Backgrounds 1 1.2. Normally-off Operation in AlGaN/GaN HFETs 3 1.3. Issues and Feasible Strategies in AlGaN/GaN MIS-HFETs 11 1.4. Research Aims 15 1.5. References 17 Chapter 2. Development and Evaluation of Low Damage Etching processes 22 2.1. Introduction 22 2.2. Various Evaluation Methods of Etching Damage 24 2.3. Low-Damage Dry Etching Methods 29 2.3.1. Inductively Coupled Plasma-Reactive Ion Etching Using BCl3/Cl2 Gas Mixture 29 2.3.2. Digital Etching Using Plasma Asher and HCl 34 2.3.3. Atomic Layer Etching Using Inductively Coupled Plasmaโ€“Reactive Ion Etching System (ICP-RIE) 50 2.4. Conclusion 75 2.5. References 76 Chapter 3. SiON/HfON Gate Dielectric Layer by ALD for AlGaN/GaN MIS-FETs 80 3.1. Introduction 80 3.2. ALD Processes for SiON and HfON 83 3.3. Electrical Characteristics of ALD SiON, HfON and SiON/HfON Dual Layer on n-GaN 87 3.4. Device Characteristics of Normally-off AlGaN/GaN MIS-FETs with SiON/HfON Dual Layer 95 3.5. Conclusion 113 3.6. References 114 Chapter 4. High Quality AlN/AlON/AlHfON Gate Dielectric Layer by ALD for AlGaN/GaN MIS-FETs 120 4.1. Introduction 120 4.2. Development of ALD AlN/AlON/AlHfON Gate Stack 122 4.2.1. Process Optimization for ALD AlN 122 4.2.2. ALD AlN as an Interfacial Layer 144 4.2.3. Thickness Optimization of AlN/AlON/ AlHfON Layer 149 4.2.4. ALD AlHfON Optimization 159 4.2.5. Material Characteristics of AlN/AlON/AlHfON Layer 167 4.3. Device Characteristics of Normally-off AlGaN/GaN MIS-FETs with AlN/AlON/AlHfON Layer 171 4.4. Conclusion 182 4.5. References 183 Chapter 5. Concluding Remarks 188 Appendix. 190 A. N2 Plasma Treatment Before Dielectric Deposition 190 B. Tri-gate Normally-on/off AlGaN/GaN MIS-FETs 200 C. AlGaN/GaN Diode with MIS-gated Hybrid Anode and Edge termination 214 Abstract in Korean 219 Research Achievements 221Docto

    Optimization of off-state breakdown voltage in GaN high-electron-mobility transistors

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    Gallium nitride (GaN) technology is the next revolution in electronics as it offers a large bandgap (high critical electric field) and high electron mobility (2D electron gas) in one transistor design, surpassing silicon (Si), gallium arsenide (GaAs), and indium phosphide (InP) based technologies. High efficiency and high voltage operation of GaN high electron mobility transistors (HEMTs) provide significant performance and size advantages over the aforementioned devices. GaN HEMTs are normally-on devices, meaning that the devices do not shut down even though no gate voltage is applied, due to the 2D electron gas channel. In applications where safety and efficiency are in the forefront, normally-off devices are preferred. A simple way to obtain a normally-off GaN HEMT is to apply a negative gate voltage. A challenge of normally-off GaN HEMT is that the devices usually fail before the critical electric field is reached. Breakdown is caused by gate-leakage impact-ionization, drain-to-source punchthrough and vertical current leakage. Increasing the breakdown voltage would eliminate the damage in high voltage, high current applications and would extend the lifetime and operating bias conditions. The goal of this research is to design and simulate GaN-based power transistors in order to understand their different characteristics, such as voltage-current relations, using TCAD Sentaurus software. GaN HEMTs with different design strategies (i.e. doping concentration, layer thicknesses, layer contents) are simulated in order to understand their impact on off-state breakdown voltages. Based on the simulation results, different strategies to improve the off-state breakdown voltage are proposed.Ope

    ANALYSIS OF FAILURE MECHANISMS THAT IMPACT SAFE OPERATION OF ALGAN/GAN HEMTS

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    The reliability of AlGaN/GaN high electron mobility transistors (HEMTs) is tra- ditionally determined via thermal lifetime acceleration stress tests. More recently it has been proposed that electric field has a prominent role in limiting lifetimes. Multi- ple failure mechanisms have been proposed as a result of device degradation observed when stressed under high applied electric fields, as typical when the device is biased into the OFF-state. One potential reason for multiple mechanisms could be due to varying levels of quality and maturity of the GaN processes in the reported literature. The work presented in this dissertation seeks to provide clarity and understanding into the failure mechanism of AlGaN/GaN HEMT devices under high electric fields. The devices in this study were fabricated in a commercial GaN process, notable for exceptional ruggedness and industry leading 65V qualified operational bias for RF power amplifiers. A series of OFF-state, high electric field step-stress experiments, as described in literature, were performed to assess if any were applicable to this process. It was discovered that device degradation could only be induced when stressed close to the breakdown limits. This lead to the development of a unique stress method that enables the device to be held close to catastrophic breakdown, while avoiding an over stress event that would prevent the device from being studied at the conclusion of the experiment. It was discovered via careful electrical and optical analysis that failure was due to a localized degradation of the Schottky gate diode properties. The physical analysis found the failure inconsistent with the widely reported inverse piezoelectric effect. Instead the failures resemble recently proposed time dependent dielectric breakdown of the AlGaN barrier laye

    Surface-potential-based compact model for the gate current of p-GaN Gate HEMTs

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    The gate leakage current of p-GaN gate HEMTs is modeled based on surface potential calculations. The model accurately describes the bias and temperature dependence of the gate leakage. Thermionic emission is the main mechanism of the gate current in forward bias operation while hopping transport component is the main mechanism of gate current in reverse bias operation. This newly developed gate current model was implemented in Verilog-A. A good agreement between the simulations and experimental data demonstrates the accuracy of the model
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