• 제목/요약/키워드: $In_xGa_{1-x}N$/GaN

검색결과 225건 처리시간 0.029초

Optimization of Ohmic Contact Metallization Process for AlGaN/GaN High Electron Mobility Transistor

  • Wang, Cong;Cho, Sung-Jin;Kim, Nam-Young
    • Transactions on Electrical and Electronic Materials
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    • 제14권1호
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    • pp.32-35
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    • 2013
  • In this paper, a manufacturing process was developed for fabricating high-quality AlGaN/GaN high electron mobility transistors (HEMTs) on silicon carbide (SiC) substrates. Various conditions and processing methods regarding the ohmic contact and pre-metal-deposition $BCl_3$ etching processes were evaluated in terms of the device performance. In order to obtain a good ohmic contact performance, we tested a Ti/Al/Ta/Au ohmic contact metallization scheme under different rapid thermal annealing (RTA) temperature and time. A $BCl_3$-based reactive-ion etching (RIE) method was performed before the ohmic metallization, since this approach was shown to produce a better ohmic contact compared to the as-fabricated HEMTs. A HEMT with a 0.5 ${\mu}m$ gate length was fabricated using this novel manufacturing process, which exhibits a maximum drain current density of 720 mA/mm and a peak transconductance of 235 mS/mm. The X-band output power density was 6.4 W/mm with a 53% power added efficiency (PAE).

Time Evolution of a High-temperature GaN Epilayer Grown on a Low-temperature GaN Buffer Layer using a Low-pressure MOCVD

  • Chang, Kyung-Hwa;Cho, Sung-Il;Kwon, Myoung-Seok
    • Transactions on Electrical and Electronic Materials
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    • 제7권1호
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    • pp.36-41
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    • 2006
  • In this paper, the time evolution of undoped GaN epilayers on a low-temperature GaN buffer layer grown on c-plane sapphire at a low pressure of 300 Torr was studied via a two-step growth condition in a horizontal MOCVD reactor. As a function of the growth time at a high-temperature, the surface morphology, structural quality, and optical and electrical properties were investigated using atomic force microscopy, high-resolution x-ray diffraction, photoluminescence, and Hall effect measurement, respectively. The root-mean-square roughness showed a drastic decrease after a certain period of surface roughening probably due to the initial island growth. The surface morphology also showed the island coalescence and the subsequent suppression of three-dimensional island nucleation. The structural quality of the GaN epilayer was improved with increasing growth time considering the symmetrical (002) and asymmetrical (102) rocking curves. The variations of room-temperature photoluminescence, background carrier concentration, and Hall mobility were measured and discussed.

GaAs 기판위에 성장된 단결정 AlAs층의 선택적 산화 및 XPS (X-ray photonelectron spectroscopy) 분석 (Selective Oxidation of Single Crystalline AlAs layer on GaAs substrate and XPS(X-ray photoelectron spectroscopy) Analysis)

  • 이석헌;이용수;태흥식;이용현;이정희
    • 센서학회지
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    • 제5권5호
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    • pp.79-84
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    • 1996
  • $n^{+}$형 GaAs 기판위에 MBE로 $1\;{\mu}m$ 두께의 GaAs층과 AlAs층 및 GaAs cap 단결정층을 차례로 성장시켰다. AlAs/GaAs epi층을 $400^{\circ}C$에서 각각 2시간 및 3시간동안 $N_{2}$로 bubbled된 $H_{2}O$ 수증기(水蒸氣)($95^{\circ}C$)에서 산화시켰다. 산화시간에 따른 산화막의 XPS 분석결과, 작은 양의 $As_{2}O_{3}$ 및 AlAS 그리고 원소형 As들이 2시간동안 산화된 시편에서 발견되었다. 그러나 3시간동안 산화시킨 후에는, 2시간동안 산화시켰을 때 산화막내에 존재하던 소량의 As 산화물과 As 원자들은 발견되지 않았다. 따라서 As-grown된 AlAs/GaAs epi층은 3시간동안 $400^{\circ}C$의 산화온도에서 선택적으로 $Al_{2}O_{3}/GaAs$으로 변화되었다. 그러므로 산화온도 및 산화시간은 AlAs/GaAs 계면에서 결함이 없는 표면을 형성하고 기판쪽으로 산화가 진행되는 것을 멈추기 위해서는 매우 결정적으로 작용하는 것으로 조사되었다.

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GaAs(100) 기판위에 성장된 AIN 박막의 특성 (The characterization of AlN thin films grown on GaAs(100) substrate)

  • 정성훈;김영호;송복식;문동찬;김선태
    • 한국전기전자재료학회:학술대회논문집
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    • 한국전기전자재료학회 1996년도 추계학술대회 논문집
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    • pp.33-36
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    • 1996
  • AIN thin films were prepared using by Rf sputtering method on the GaAs(170) substrate and investigated by X-ray diffractometer, IR spectroscopy, n&k system. The parameters were the substrate temperature, RF power, sputtering duration and the $N_2$/Ar ratio. The AlN thin films of (101) orientation were obtained under the conditions of room temperature and the nitrogen of 60 vol.%. The crystallinity of the films, which were grown respectively under the different conditions, were determined by the comparison of the band width of an E$_1$[TO:680$cm^{-1}$ /] phonon mode. The thicknesses of AlN films were decreased dramatically in the region of the nitrogen of 40~60 vol.% according to the increment of the $N_2$/Ar ratio by which the sputter yield got lower.

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Direct Imaging of Polarization-induced Charge Distribution and Domain Switching using TEM

  • 오상호
    • 한국진공학회:학술대회논문집
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    • 한국진공학회 2013년도 제45회 하계 정기학술대회 초록집
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    • pp.99-99
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    • 2013
  • In this talk, I will present two research works in progress, which are: i) mapping of piezoelectric polarization and associated charge density distribution in the heteroepitaxial InGaN/GaN multi-quantum well (MQW) structure of a light emitting diode (LED) by using inline electron holography and ii) in-situ observation of the polarization switching process of an ferroelectric Pb(Zr1-x,Tix)O3 (PZT) thin film capacitor under an applied electric field in transmission electron microscope (TEM). In the first part, I will show that strain as well as total charge density distributions can be mapped quantitatively across all the functional layers constituting a LED, including n-type GaN, InGaN/GaN MQWs, and p-type GaN with sub-nm spatial resolution (~0.8 nm) by using inline electron holography. The experimentally obtained strain maps were verified by comparison with finite element method simulations and confirmed that not only InGaN QWs (2.5 nm in thickness) but also GaN QBs (10 nm in thickness) in the MQW structure are strained complementary to accommodate the lattice misfit strain. Because of this complementary strain of GaN QBs, the strain gradient and also (piezoelectric) polarization gradient across the MQW changes more steeply than expected, resulting in more polarization charge density at the MQW interfaces than the typically expected value from the spontaneous polarization mismatch alone. By quantitative and comparative analysis of the total charge density map with the polarization charge map, we can clarify what extent of the polarization charges are compensated by the electrons supplied from the n-doped GaN QBs. Comparison with the simulated energy band diagrams with various screening parameters show that only 60% of the net polarization charges are compensated by the electrons from the GaN QBs, which results in the internal field of ~2.0 MV cm-1 across each pair of GaN/InGaN of the MQW structure. In the second part of my talk, I will present in-situ observations of the polarization switching process of a planar Ni/PZT/SrRuO3 capacitor using TEM. We observed the preferential, but asymmetric, nucleation and forward growth of switched c-domains at the PZT/electrode interfaces arising from the built-in electric field beneath each interface. The subsequent sideways growth was inhibited by the depolarization field due to the imperfect charge compensation at the counter electrode and preexisting a-domain walls, leading to asymmetric switching. It was found that the preexisting a-domains split into fine a- and c-domains constituting a $90^{\circ}$ stripe domain pattern during the $180^{\circ}$ polarization switching process, revealing that these domains also actively participated in the out-of-plane polarization switching. The real-time observations uncovered the origin of the switching asymmetry and further clarified the importance of charged domain walls and the interfaces with electrodes in the ferroelectric switching processes.

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nBn Based InAs/GaSb Type II Superlattice Detectors with an N-type Barrier Doping for the Infrared Detection

  • 김하술;이훈;황제환;이상준
    • 한국진공학회:학술대회논문집
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    • 한국진공학회 2014년도 제46회 동계 정기학술대회 초록집
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    • pp.128.2-128.2
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    • 2014
  • Long-wave infrared detectors using the type-II InAs/GaSb strained superlattice (T2SL) material system with the nBn structure were designed and fabricated. The band gap energy of the T2SL material was calculated as a function of the thickness of the InAs and GaSb layers by the Kronig-Penney model. Growth of the barrier material (Al0.2Ga0.8Sb) incorporated Te doping to reduce the dark current. The full width at half maximum (FWHM) of the 1st satellite superlattice peak from the X-ray diffraction was around 45 arc sec. The cutoff wavelength of the fabricated device was ${\sim}10.2{\mu}m$ (0.12eV) at 80 K while under an applied bias of -1.4V. The measured activation energy of the device was ~0.128 eV. The dark current density was shown to be $1.2{\times}10^{-5}A/cm^2$ at 80 K and with a bias -1.4 V. The responsivity was 1.9 A/W at $7.5{\mu}m$ at 80K and with a bias of -1.9V.

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MATERIALS AND DETECTORS BASED ON GaInAs GROWN BY HYDRIDE VPE TECHNIQUE UTILIQUE UTILIZING A Ga/IN ALLOY SOURCE

  • Park, Chin-Ho;Tiothy J.Anderson
    • 한국진공학회지
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    • 제4권S1호
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    • pp.168-173
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    • 1995
  • $GaxIn{1_x}As$ epitaxial layers were grown by a simplified hydrode vapor phase epitaxy(VPE) method bsed on the utilization of Ga/In alloy as the source metal. The effects of a wide range of experimental variables(i.e.,inlet mole fraction of HCI, deposition temperature, Ga/In alloy composition) on the ternary composition and growth rate were investigated. Layers of $Ga_{0.47}In_{0.53}As$ lattice matched to InP were successfully grown from alloys containing 5 to 8 at.% Ga. These layers were used to produce state-of-the art p-i-n photodetectors having the following characteristics: dark current, $I_d$(-5V) = 10-20 nA: responsivity, R=0.84-0.86 A/W; dark current, Id(-5V)=10-20 nA; responsivity, R=0.84-0.86 A/W; capacitance, C=0.88-0.92 pF; breakdown voltage, $V_b$ >40V. This study demonstrated for the first time that a simplified hydride VPE process with a Ga/In alloy source is capable of producing device quality epitaxial layers.

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1.55 $1.55{\mu}m$ InGaAsP/InGaAsP MQW 광흡수 변조기에서 구조변수가 소광특성에 미치는 영향 (Structural dependences of the extinction in an 1.55 $1.55{\mu}m$ InGaAsP/InGaAsP multiple-quantum-well electro-absorption modulator)

  • 민영선;심종인;어영선
    • 한국광학회지
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    • 제12권1호
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    • pp.40-47
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    • 2001
  • 초고속 디지털 광통신용 $1.55{\mu}m$ InGaAsP/InGaAsP MQW 광흡수 변조기에서 각종 구조변수들이 광흡수변조기 성능에 미치는 영향을 체계적으로 조사분석하였다. 일반적으로 행하여지는 양자우물 수 $N_w$, 양자우물 두께 $t_w$, detuning 양 $\Delta\lambda$, 소자길이 L과 같은 구조 파라미터들에 더불어 본 연구에서 새롭게 제안한 SCH 영역내에 n형으로 도핑된 길이 $t_n$가 소자 성능에 미치는 영향을 해석하였다 이를 통해 소자길이 L=$100{\mu}m$의 광흡수변조기에서 구동 전압 $V_{\alpha}$=0~-2V 영역에서 동작하고 기초흡수 -1.5dB 이하, -1V에서 -2.92dB 및 -2V에서 -10.0dB 이상의 소광비를 주는 우수한 성능을 갖는 초고속 광흡수 변조기 설계가 가능하였다.

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유전체덮개 양자우물 무질서공정에서 $SiN_{x}$ 덮개층 성장시 $NH_3$ 유량비 조절을 통한 InGaAs/InGaAsP 양자우물의 밴드갭 조절

  • 최원준;이희택;우덕하;이석;김선호;조재원
    • 한국광학회:학술대회논문집
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    • 한국광학회 2000년도 제11회 정기총회 및 00년 동계학술발표회 논문집
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    • pp.256-257
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    • 2000
  • 유전체 덮개층을 이용한 impurity free vacancy disordering (IFVD) 기술에 의한 양자우물구조의 밴드갭 조절기술은 양자우물을 갖는 광소자의 제작 및 광소자들의 한판 집적에 광범위하게 적용되어 왔다$^{(1-3)}$ . IFVD 기술의 핵심은 유전체 덮개층의 종류 및 그 특성을 적절히 조절함으로써 양자우물의 밴드갭 및 굴절율을 양자우물 기판상에서 공간적으로 조절하는 기술에 있다. 이러한 목적을 위해 SiN$_{x}$ , SiO$_2$, SrF$_2$ 및 WN$_{x}$ 와 같은 많은 유전체 덮개층에 관한 실험들이 진행되었다 $^{(1-6)}$ . (중략)

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