• Title/Summary/Keyword: Low temperature GaN

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GaN Nanowire Growth on Si Substrate by Utilizing MOCVD Methods (MOCVD 방법에 의한 Si 기판위 GaN 나노선의 성장)

  • Woo, Shi-Gwan;Shin, Dae-Keun;O, Byung-Sung;Lee, Hyung-Gyoo
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.23 no.11
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    • pp.848-853
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    • 2010
  • We have grown GaN nanowires by the low pressure MOCVD method on Ni deposited oxidized Si surface and have established optimum conditions by observing surface microstructure and its photoluminescence. Optimum growth temperature of $880^{\circ}C$, growth time of 30 min, TMG source flow rate of 10 sccm have resulted in dense nanowires on the surface, however further increase of growth time or TMG flow rate has not increased the length of nanowire but has formed nanocrystals. On the contrary, the increase of ammonia flow has increased the length of nanowires and the coverage of nanowire over the surface. The shape of nanowire is needle-like with a Ni droplet at its tip; the length is tens of micron with more than 40 nm in diameter. Low temperature photoluminescence obtained from the sample at optimum growth condition has revealed several peaks related to exciton decay near band-edge, but does not show any characteristic originated from one dimensional quantum confinement. Strong and broad luminescence at 2.2 eV is observed from dense nanowire samples and this suggests that the broad band is related to e-h recombination at the surface state in a nanowire. The current result is implemented to the nanowire device fabrication by nanowire bridging between micro-patterned neighboring Ni catalysis islands.

Free exciton transitions and Varshni′s coeffecients for GaN epitaxial layers grown by horizontal LP - MOCVD

  • Lee, Joo-in;Leem, Jae-Young;Son, J.S.;Viswanath, A. Kasi
    • Journal of Korean Vacuum Science & Technology
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    • v.4 no.3
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    • pp.63-67
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    • 2000
  • We have studied the photoluminescence properties of undoped epitaxial layers of GaN on sapphire substrate grown by horizontal low pressure metal organic chemical vapor deposition method in the temperature range of 9-300 K. At 9 K the spectra are dominated by the well resolved interband free excitons A and B as well as bound excitons. Temperature dependence of free exciton transitions was studied and Varshni's coefficients for the temperature variation of bandgap were determined.

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Ultraviolet LEDs using n-ZnO:Ga/i-ZnO/p-GaN:Mg heterojunction (n-ZnO/i-ZnO/p-GaN:Mg 이종접합을 이용한 UV 발광 다이오드)

  • Han, W.S.;Kim, Y.Y.;Kong, B.H.;Cho, H.K.;Lee, J.H.;Kim, H.S.
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2008.11a
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    • pp.50-50
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    • 2008
  • ZnO has been extensively studied for optoelectronic applications such as blue and ultraviolet (UV) light emitters and detectors, because it has a wide band gap (3.37 eV) anda large exciton binding energy of ~60 meV over GaN (~26 meV). However, the fabrication of the light emitting devices using ZnO homojunctions is suffered from the lack of reproducibility of the p-type ZnO with high hall concentration and mobility. Thus, the ZnO-based p-n heterojunction light emitting diode (LED) using p-Si and p-GaN would be expected to exhibit stable device performance compared to the homojunction LED. The n-ZnO/p-GaN heterostructure is a good candidate for ZnO-based heterojunction LEDs because of their similar physical properties and the reproducibleavailability of p-type GaN. Especially, the reduced lattice mismatch (~1.8 %) and similar crystal structure result in the advantage of acquiring high performance LED devices with low defect density. However, the electroluminescence (EL) of the device using n-ZnO/p-GaN heterojunctions shows the blue and greenish emissions, which are attributed to the emission from the p-GaN and deep-level defects. In this work, the n-ZnO:Ga/p-GaN:Mg heterojunction light emitting diodes (LEDs) were fabricated at different growth temperatures and carrier concentrations in the n-type region. The effects of the growth temperature and carrier concentration on the electrical and emission properties were investigated. The I-V and the EL results showed that the device performance of the heterostructure LEDs, such as turn-on voltage and true ultraviolet emission, developed through the insertion of a thin intrinsic layer between n-ZnO:Ga and p-GaN:Mg. This observation was attributed to a lowering of the energy barriers for the supply of electrons and holes into intrinsic ZnO, and recombination in the intrinsic ZnO with the absence of deep level emission.

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Electrically Driven Quantum Dot/wire/well Hybrid Light-emitting Diodes via GaN Nano-sized Pyramid Structure

  • Go, Yeong-Ho;Kim, Je-Hyeong;Kim, Ryeo-Hwa;Go, Seok-Min;Gwon, Bong-Jun;Kim, Ju-Seong;Kim, Taek;Jo, Yong-Hun
    • Proceedings of the Korean Vacuum Society Conference
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    • 2011.02a
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    • pp.47-47
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    • 2011
  • There have been numerous efforts to enhance the efficiency of light-emitting diodes (LEDs) by using low dimensional structures such as quantum dots (QDs), wire (QWRs), and wells (QWs). We demonstrate QD/QWR/QW hybrid structured LEDs by using nano-scaled pyramid structures of GaN with ~260 nm height. Photoluminescence (PL) showed three multi-peak spectra centered at around 535 nm, 600 nm, 665 nm for QWs, QWRs, and QDs, respectively. The QD emission survived at room temperature due to carrier localization, whereas the QW emission diminished from 10 K to 300 K. We confirmed that hybrid LEDs had zero-, one-, and two-dimensional behavior from a temperature-dependent time-resolved PL study. The radiative lifetime of the QDs was nearly constant over the temperature, while that of the QWs increased with increasing temperature, due to low dimensional behavior. Cathodoluminescence revealed spatial distributions of InGaN QDs, QWRs, and QWs on the vertices, edges, and sidewalls, respectively. We investigated the blue-shifted electroluminescence with increasing current due to the band-filling effect. The hybrid LEDs provided broad-band spectra with high internal quantum efficiency, and color-tunability for visible light-emitting sources.

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Analysis for Buffer Leakage Current of High-Voltage GaN Schottky Barrier Diode (고전압 GaN 쇼트키 장벽 다이오드의 완충층 누설전류 분석)

  • Hwang, Dae-Won;Ha, Min-Woo;Roh, Cheong-Hyun;Park, Jung-Ho;Hahn, Cheol-Koo
    • Journal of the Institute of Electronics Engineers of Korea SD
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    • v.48 no.2
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    • pp.14-19
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    • 2011
  • We have fabricated GaN Schottky barrier diode (SBD) for high-voltage applications on Si substrate. The leakage current and the electrical characteristics of GaN SBD are investigated by annealing metal-semiconductor junctions. Ohmic junctions of Ti/Al/Mo/Au and Schottky junctions of Ni/Au are used in the fabrication. A test structure is proposed to measured buffer leakage current through a mesa structure. When annealing temperature is increased from $700^{\circ}C$ to $800^{\circ}C$, measured buffer leakage current is also increased from 87 nA to 780 nA at the width of 100 ${\mu}m$. The diffusion of Au, Ti, Mo, O into GaN buffer layer increases the leakage current and that is verified by Auger electron spectroscopy. Experimental results show that the low leakage current and the high breakdown voltage of GaN SBD are achieved by annealing metal-semiconductor junctions.

Formation of Vanadium-based Ohmic Contacts to n-GaN (n-GaN/vanadium-based Ohmic 접촉 형성)

  • Song, June-O;Leem, Dong-Seok;Kim, Sang-Ho;Seong, Tae-Yeon
    • Korean Journal of Materials Research
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    • v.13 no.9
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    • pp.567-571
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    • 2003
  • We investigate vanadium (V)-based Ohmic contacts on n-GaN ($N_{d}$=$2.0${\times}$10^{18}$ $cm^{-3}$ ) as a function of annealing temperature. It is shown that the V (60 nm) contacts become Ohmic with specific contact resistances of $10^{-3}$ $- 10^{-4}$$\textrm{cm}^2$ upon annealing at 650 and $850^{\circ}C$. The V(20 nm)/Ti(60 nm)/Au(20 nm)contacts produce very low specific contact resistances of $2.2 ${\times}$ 10^{-5}$ and$ 4.0${\times}$10^{-6}$$\textrm{cm}^2$ when annealed at 650 and $850{\circ}C$, respectively. A comparison shows that the use of the overlayers (Ti/Au) is very effective in improving Ohmic property. Based on the current-voltage measurement, Auger electron spectroscopy, glancing angle X-ray diffraction, and X-ray photoemission spectroscopy results, the possible mechanisms for the annealing temperature dependence of the Ohmic behavior of the V-based contacts are described and discussed.d.

Change in Electrical Properties of Al2O3/GaN MIS Structures according to the Thickness of Al2O3 Thin Film and Annealing Temperature (산화알루미늄 박막의 두께 및 열처리 온도에 따른 Al2O3/GaN MIS 구조의 전기적 특성 변화)

  • Kwak, No-Won;Lee, Woo-Seok;Kim, Ka-Lam;Kim, Hyun-Jun;Kim, Kwang-Ho
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.22 no.6
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    • pp.470-475
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    • 2009
  • We deposited $Al_2O_3$ thin films on GaN by remote plasma atomic layer deposition (RPALD) technique, trimethylaluminum(TMA) and oxygen were used as precursors, at fixed process condition, the number of cycle were changed. Growth rate per cycle was $1.2\;{\AA}$/cycle. and Growth rate was in proportion to a number of cycle, the GaN MIS capacitors that $Al_2O_3$ thin film were deposited above 12 nm, have excellent electrical properties, a low electrical leakage current density(${\sim}10^{-10}\;A/cm^2$ at 1.5 MV), but below 12 nm, we can see the degradation of the leakage current density. After post deposition annealing, Dielectric constant was estimated by 1 MHz high-frequency C-V method, it was varied with the anealing temperature from 6.9 at no post anealed to 7.6 at $800^{\circ}C$, and we can see a improvement of the leakage current density and breakdown voltage by post deposition anealing below $700^{\circ}C$, but, after anealed at $800^{\circ}C$, we can see the degradation of the leakage current density and breakdown voltage.

The growth of GaN on the metallic compound graphite substrate by HVPE (HVPE 방법에 의한 금속 화합물 탄소체 기판 위의 GaN 성장)

  • Kim, Ji Young;Lee, Gang Seok;Park, Min Ah;Shin, Min Jeong;Yi, Sam Nyung;Yang, Min;Ahn, Hyung Soo;Yu, Young Moon;Kim, Suck-Whan;Lee, Hyo Suk;Kang, Hee Shin;Jeon, Hun Soo;Sawaki, Nobuhiko
    • Journal of the Korean Crystal Growth and Crystal Technology
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    • v.23 no.5
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    • pp.213-217
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    • 2013
  • The GaN layer was typical III-V nitride semiconductor and was grown on the sapphire substrate which cheap and convenient. However, sapphire substrate is non-conductivity, low thermal conductivity and has large lattice mismatch with the GaN layer. In this paper, the poly GaN epilayer was grown by HVPE on the metallic compound graphite substrate with good heat dissipation, high thermal and electrical conductivity. We tried to observe the growth mechanism of the GaN epilayer grown on the amorphous metallic compound graphite substrate. The HCl and $NH_3$ gas were flowed to grow the GaN epilayer. The temperature of source zone and growth zone in the HVPE system was set at $850^{\circ}C$ and $1090^{\circ}C$, respectively. The GaN epilayer grown on the metallic compound graphite substrate was observed by SEM, EDS, XRD measurement.

Studies on the growth and properties of orthophosphate crystals by the hydrothermal method (수열법에 의한 올소인산염 결정의 육성과 성질에 관한 연구)

  • Pan-Chae Kim
    • Journal of the Korean Crystal Growth and Crystal Technology
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    • v.4 no.2
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    • pp.139-147
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    • 1994
  • Orthophosphate crystals were grown by the hydrothermal method and the properties of grown crystals were investigated by means of X-ray diffraction. Vickers hardness tester, etc. The starting powders of $AIPO_4 and GaPO_4 $were prepared as a single phase by the solid state reaction of stoichiometric mixture of $AI_2O_3 or Ga_2O_3$ and $NH_4H_2PO_4$ and the subsequently by the hydrothermal treatment. The hydrothermal conditions for high growth rates of the orthophosphate crystals are as follows: $AlPO_4$ crystal; temperature ranges, between $170$~$200^{\circ}C$; temperatures difference, $15$~$20^{\circ}C;$, hydrothermal solvent, 4m HCl, $GaPO_4 crystal; temperature ranges, between $210 and 240^{\circ}C;$; temperature difference, $25$~$30^{\circ}C; $, hydrothermal solvent, 4m HCl. Morphologies of grown crystals tended to be bounded by (1010), (1011) and (0111) faces at low temperatures, and grew with well developed (0001) faces by increasing the growth temperature. On the other hand, the properties of orthophosphate crystals $(AlPO_4/GaPO_4)$ were as follows: lattice parameters (nm); a=0.494, c=1.094/a=0.490, c=1.105, density (gcm-3); 2.62/3.56, Vickers hardness (Nm^2); $1.02{\times}10^1^0/7.06{\times}10^9$, refractive indices; $ne=1.529{\pm}0.003, no=1.519{\pm}0.003/ne=1.611{\pm}0.006, no=1.599{\pm}0.006, birefringence; {\pm}0.01/{\pm}0.012$, dielectric constant (Fm-1); 6/7.

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SiO2 보호막 증착에 따른 p-GaN의 후열처리 효과 연구

  • Park, Jin-young;Ji, Taeksoo;Lee, Jin-hong;An, Su-chang
    • Proceedings of the Korean Institute of Information and Commucation Sciences Conference
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    • 2013.05a
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    • pp.772-775
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    • 2013
  • We have grown a p-GaN film on sapphire by MOCVD and explored the post-annealing effort on the film after depositing a $2500{\AA}$ thick $SiO_2$ protective layer on it. By etching the $SiO_2$ protective film after the heat treatment, the hole concentration was measured, and compared with the data values before the heat treatment. In addition to the concentration, the hole mobility was also monitored while varying the atmospheric gas ratio of $N_2$ and $O_2$, the rapid thermal annealing temperatures ($750^{\circ}C$ and $650^{\circ}C$) and times (1 to 15 min.) In order to investigate the optical and structural properties of the film, room temperature and low temperature PL measurements were conducted.

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