• Title/Summary/Keyword: AlGaN/GaN. heterostructure

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Composition and interface quality control of AlGaN/GaN heterostructure and their 2DEG transport properties

  • Kee, Bong;Kim, H.J.;Na, H.S.;Kwon, S.Y.;Lim, S.K.;Yoon, Eui-Joon
    • Journal of Korean Vacuum Science & Technology
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    • v.4 no.3
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    • pp.81-85
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    • 2000
  • The effects of $NH_3$ flow rate and reactor pressure on Al composition and the interface of AlGaN/GaN heterostructure were studied. Equilibrium partial pressure of Ga and Al over AiGaN alloy was calculated as a function of growth pressure, $NH_3$flow rate and temperature. It was found equilbrium vapor pressure of Al is significantly lower than that of Ga, thus, the alloy composition mainly controlled by Ga partial pressure. We believe that more decomposition of Ga occur at lower $NH_3$ flow rate and higher growth pressure leads to preferred Al incorporation into AlGaN. The alloy composition gradient became larger at AlGaN/GaN heterointerface at higher reactor pressures, higher Al composition and low $NH_3$ flow rate. This composition gradient lowered sheet carrier concentration and electron mobility as well. We obtained an AlGaN/GaN heterostructure with sheet carrier density of ${\sim}2{\times}10^{13}cm^{-2}$ and mobility of 1250 and 5000 $cm^2$/Vs at 300 K and 100 K, respectively.

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High Sensitivity Hydrogen Sensor Based on AlGaN/GaN-on-Si Heterostructure (AlGaN/GaN-on-Si 이종접합 기반의 고감도 수소센서)

  • Choi, June-Heang;Jo, Min-Gi;Kim, Hyungtak;Lee, Ho-Kyoung;Cha, Ho-Young
    • KEPCO Journal on Electric Power and Energy
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    • v.5 no.1
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    • pp.39-43
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    • 2019
  • Hydrogen energy has positive effects as an alternative energy source to overcome the energy shortage issues. On the other hand, since stability is very important in use, sensor technology that enables accurate and rapid detection of hydrogen gas is highly required. In this study, hydrogen sensor was developed on AlGaN/GaN heterostructure platform using Pd catalyst where a recess structure was employed to improve the sensitivity. Temperature and bias voltage dependencies on sensitivity were carefully investigated using a hydrogen concentration of 4% that is the safety threshold concentration. Due to the excellent properties of AlGaN/GaN heterostructure in conjunction with the recess structure, a very high sensitivity of 56% was achieved with a fast response speed of 0.75 sec.

Characteristics of selective area growth of GaN/AlGaN double heterostructure grown by hydride vapor phase epitaxy on r-plane sapphire substrate (HVPE 방법에 의해 r-plane 사파이어 기판 위의 선택 성장된 GaN/AlGaN 이종 접합구조의 특성)

  • Hong, S.H.;Jeon, H.S.;Han, Y.H.;Kim, E.J.;Lee, A.R.;Kim, K.H.;Hwang, S.L.;Ha, H.;Ahn, H.S.;Yang, M.
    • Journal of the Korean Crystal Growth and Crystal Technology
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    • v.19 no.1
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    • pp.6-10
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    • 2009
  • In this paper, a selective area growth (SAG) of a GaN/AlGaN double heterostructure (DH) has been performed on r-plane sapphire substrate by using the mixed-source hydride vapor phase epitaxy (HVPE) with multi-sliding boat system. The SAG-GaN/AlGaN DH consists of GaN buffer layer, Te-doped AlGaN n-cladding layer, GaN active layer, Mg-doped AlGaN p-cladding layer, and Mg-doped GaN p-capping layer. The electroluminescence (EL) characteristics show an emission peak of wavelength, 439 nm with a full width at half maximum (FWHM) of approximately 0.64 eV at 20 mA. The I-V measurements show that the turn-on voltage of the SAG-GaN/AlGaN DH is 3.4 V at room temperature. We found that the mixed-source HVPE method with a multi-sliding boat system was one of promising growth methods for III-Nitride LEDs.

Deformation of the AlGaN/GaN metal-oxide-semiconductor heterostructure field-effect transistor characteristics by UV irradiation

  • Lim, Jin Hong;Kim, Jeong Jin;Yang, Jeon Wook
    • Journal of IKEEE
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    • v.17 no.4
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    • pp.531-536
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    • 2013
  • The impact of UV irradiation process on the AlGaN/GaN metal-oxide-semiconductor heterostructure field-effect transistor was investigated. Due to the high intensity UV irradiation before the gate dielectric deposition, the conductivity of AlGaN/GaN structure and the drain saturation current of the transistor increased by about 10 %. However, the pinch off characteristics of transistor was severely deformed by the process. By comparing the electrical characteristics of the transistors, it was proposed that the high intensity UV irradiation formed a sub-channel under the two dimensional electron gas of AlGaN/GaN structure even without additional impurity injection.

NO2 gas sensor using an AlGaN/GaN Heterostructure FET with SnO2 catalyst deposited by ALD technique (원자막증착법(ALD) SnO2 촉매를 적용한 AlGaN/GaN 이종접합 트랜지스터 NO2 가스센서)

  • Yang, Suhyuk;Kim, Hyungtak
    • Journal of IKEEE
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    • v.24 no.4
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    • pp.1117-1121
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    • 2020
  • In this work, it was confirmed that a SnO2 catalyst deposited by an atomic layer deposition(ALD) process can be employed in AlGaN/GaN heterostructure FET to detect NO2 gas. The fabricated HFET sensors on AlGaN/GaN-on-Si platform demonstrated that the devices with or without n-situ SiN have sensitivity of 5.5 % and 38 % at 200 ℃, respectively with response to 100 ppm-NO2.

Investigation of Buffer Traps in AlGaN/GaN Heterostructure Field-Effect Transistors Using a Simple Test Structure

  • Jang, Seung Yup;Shin, Jong-Hoon;Hwang, Eu Jin;Choi, Hyo-Seung;Jeong, Hun;Song, Sang-Hun;Kwon, Hyuck-In
    • JSTS:Journal of Semiconductor Technology and Science
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    • v.14 no.4
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    • pp.478-483
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    • 2014
  • We propose a new method which can extract the information about the electronic traps in the semi-insulating GaN buffer of AlGaN/GaN heterostructure field-effect transistors (HFETs) using a simple test structure. The proposed method has a merit in the easiness of fabricating the test structure. Moreover, the electric fields inside the test structure are very similar to those inside the actual transistor, so that we can extract the information of bulk traps which directly affect the current collapse behaviors of AlGaN/GaN HEFTs. By applying the proposed method to the GaN buffer structures with various unintentionally doped GaN channel thicknesses, we conclude that the incorporated carbon into the GaN back barrier layer is the dominant origin of the bulk trap which affects the current collapse behaviors of AlGaN/GaN HEFTs.

Optically Pumped Stimulated Emission from AlGaN/GaN Double-Heterostructure (AlGaN/GaN이중 이종접합구조의 광여기 유도방출 특성)

  • Kim, Seon-Tae;Mun, Dong-Chan
    • Korean Journal of Materials Research
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    • v.5 no.4
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    • pp.445-450
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    • 1995
  • AIN 완충층을 이용하여 대기압 유기금속에피텍셜 (MOVPE)법으로 사파이어 기판위에 성장시킨 AlGaN/GaN 이중 이종접합구조(double heterostructure : DH)의 고밀도 광여기에 의한 자외선 영역에서의 단면모드 유도방출 특성에 대하여 조사하였다. 실온에서 여기광 밀도 200kW/$cm^{2}$에서 방출된 AlGaN/GaN DH의 유도방출 피크파장과 반치폭은 각각 369nm와 22.4meV이었으며, 80K의 온도에서는 각각 360.1nm와 13.4meV이었다. 고밀도 광여기에 의하여 단면모드 자외영역 유도방출을 얻기에 필요한 입사광 밀도의 임계치는 실온과 80K의 온도에서 각각 89kW/$cm^{2}$와 44kW/$cm^{2}$이었다.

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Poperties of Optically Pumped Stimulated Emission and its Polarization from an AlGaN/GaInN Double Heterostructure (AlGaN/GaInN 이중 이종접합구조의 광여기 유도방출과 편광특성)

  • Kim, Seon-Tae;Mun, Dong-Chan
    • Korean Journal of Materials Research
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    • v.5 no.4
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    • pp.420-425
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    • 1995
  • AlGaN/GaInN 이중이종접합구조(double heterostructure :DH)를 대기압 유기금속기상에 피텍셜(MOVPE)법으로 AIN 와충층을 이용하여 사파이어 기판위에 성장하고, 실온에서의 광여기법에 의한 청색영역의 단면모드 유도방출특성과 편광특성을 조사하였다. 여기광원의 광밀도가 증가함에 따라 청색 영역에서의 유도방출 피크는 낮은 에너지 쪽으로 이동하였고, 유도방출 피크파장은 여기광밀도가 200kW/$cm^{2}$일때 402nm 이었으며, 스펙트럼의 반치폭은 18meV 이었다. 또한 유도방출에 필요한 여기광밀도의 임계치는 130 kW/$cm^{2}$ 이었다. AlGaN/GaInN로부터 방출되는 유도방출 광은 임계치 이상에서 TE-mode로 편광 되었다.

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Electrics and Noise Performances of AlGaN/GaN HEMTs with/without In-situ SiN Cap Layer (In-situ SiN 패시베이션 층에 따른 AlGaN/GaN HEMTs의 전기적 및 저주파 잡음 특성)

  • Yeo Jin Choi;Seung Mun Baek;Yu Na Lee;Sung Jin An
    • Journal of Adhesion and Interface
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    • v.24 no.2
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    • pp.60-63
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    • 2023
  • The AlGaN/GaN heterostructure has high electron mobility due to the two-dimensional electron gas (2-DEG) layer, and has the characteristic of high breakdown voltage at high temperature due to its wide bandgap, making it a promising candidate for high-power and high-frequency electronic devices. Despite these advantages, there are factors that affect the reliability of various device properties such as current collapse. To address this issue, this paper used metal-organic chemical vapor deposition to continuously deposit AlGaN/GaN heterostructure and SiN passivation layer. Material and electrical properties of GaN HEMTs with/without SiN cap layer were analyzed, and based on the results, low-frequency noise characteristics of GaN HEMTs were measured to analyze the conduction mechanism model and the cause of defects within the channel.

HVPE growth of GaN/InGaN heterostructure on r-plane sapphire substrate (R-plane 사파이어 기판위의 GaN/InGaN 이종접합구조의 HVPE 성장)

  • Jeon, H.S.;Hwang, S.L.;Kim, K.H.;Jang, K.S.;Lee, C.H.;Yang, M.;Ahn, H.S.;Kim, S.W.;Jang, S.H.;Lee, S.M.;Park, G.H.;Koike, M.
    • Journal of the Korean Crystal Growth and Crystal Technology
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    • v.17 no.1
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    • pp.6-10
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    • 2007
  • The a-plane GaN layer on r-plane $Al_2O_3$ substrate is grown by mixed-source hydride vapor phase epitaxy (HVPE). The GaN/InGaN heterostructure is performed by selective area growth (SAG) method. The heterostructure consists of a flown over mixed-sourec are used as gallium (or indium) and nitrogen sources. The gas flow rates of HCl and $NH_3$ are maintained at 10 sccm and 500 sccm, respectively. The temperatures of GaN source zone is $650^{\circ}C$. In case of InGaN, the temperature of source zone is $900^{\circ}C$. The grown temperatures of GaN and InGaN layer are $820^{\circ}C\;and\;850^{\circ}C$, respectively. The EL (electroluminescence) peak of GaN/InGaN heterostructure is at nearly 460 nm and the FWHM (full width at half maximum) is 0.67 eV. These results are demonstrated that the heterostructure of III-nitrides on r-plane sapphire can be successfully grown by mixed-source HVPE with multi-sliding boat system.