• Proceedings of the Korean Vacuum Society Conference
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• 2010.08a
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• pp.231-231
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• 2010

GaN는 상온에서 3.4 eV의 넓은 밴드갭을 갖는 직접천이형 반도체로 우수한 전기적/광학적 특성 및 화학적 안정성으로 발광 다이오드 및 레이저 다이오드 등과 같은 광전소자 응용을 위한 소재로 많은 연구가 진행되어왔다. 특히, GaN 나노구조의 경우 낮은 결함밀도, 빠른 구동 및 고집적 특성 등을 가지기 때문에 효과적으로 소자의 광학적/전기적 특성을 향상시킬 수 있어 나노구조 성장을 위한 연구가 활발히 진행되고 있다. 최근에는 Metal organic vapor deposition (MOCVD), hot filament chemical vapor deposition (CVD), molecular beam epitaxy (MBE), hydride vapor phase epitaxy (HVPE) 등 다양한 방법을 통해 성장된 GaN 나노구조가 보고되고 있다. 하지만 고가 장비 사용 및 높은 공정 온도, 복잡한 공정과정이 요구되며 크기조절, 조성비, 도핑 등과 같은 해결되어야 할 문제가 여전히 남아있다. 본 연구에서는 나노구조를 형성하기 위하여 보다 간단한 방법인 전기화학증착법을 이용하여 GaN 나노구조를 ITO 및 FTO가 증착된 전도성 glass 기판 위에 성장하였고 성장 메커니즘 및 그 특성을 분석하였다. GaN 나노구조는 gallium nitrate와 ammonium nitrate가 혼합된 전해질 용액에 Pt mesh 구조 및 전도성 glass 기판을 1cm의 거리를 유지하도록 담가두고 일정한 전압을 인가하여 성장시켰다. Pt mesh 구조 및 전도성 glass 기판은 각각 상대전극 (counter electrode) 및 작업전극 (working electrode)으로 사용되었고 전해질 용액의 농도, 인가전압, 성장시간 등의 다양한 조건을 통하여 GaN 나노구조를 성장하고 분석하였다. 성장된 GaN 나노구조 및 형태는 field emission scanning electron microscopy (FE-SEM)를 이용하여 분석하였고, energy dispersive X-ray (EDX) 분석을 통하여 정량 및 정성적 분석을 수행하였다. 그리고 성장된 GaN 나노구조의 결정성을 조사하기 위해 X-ray diffraction (XRD)을 측정 및 분석하였다. 또한, photoluminescence (PL) 분석으로부터 GaN 나노구조의 광학적 특성을 분석하였다.

• Journal of Sensor Science and Technology
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• v.24 no.1
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• pp.15-21
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• 2015

Transparent and conductive multilayer thin films consisting of three alternating layers FZTO/Ag/$WO_3$ have been fabricated by radio-frequency (RF) sputtering for the applications as transparent conducting oxides and the structural and optical properties of the resulting films were carefully studied. The single layer fluorine doped zinc tin oxide (FZTO) and tungsten oxide ($WO_3$) films grown at room temperature are found to have an amorphous structure. Multilayer structured electrode with a few nm Ag layer embedded in FZTO/Ag/$WO_3$ (FAW) was fabricated and showed the optical transmittance of 87.60 % in the visible range (${\lambda}=380{\sim}770nm$), quite low electrical resistivity of ${\sim}10^{-5}{\Omega}cm$ and the corresponding figure of merit ($T^{10}/R_s$) is equivalent to $3.0{\times}10^{-2}{\Omega}^{-1}$. The resultant power conversion efficiency of 2.50% of the multilayer based OPV is lower than that of the reference commercial ITO. Asymmetric D/M/D multilayer is a promising transparent conducting electrode material due to its low resistivity, high transmittance, low temperature deposition and low cost components.

• Proceedings of the Korean Vacuum Society Conference
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• 2011.08a
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• pp.341-341
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• 2011

최근 AMOLED 구동이 가능한 소자에 대한 연구가 활발히 진행중이다. AMOLED구동 가능소자는 LTPS TFT, a-Si TFT, OTFT, Oxide TFT가 있으며 그 중에서 현재 대부분 LTPS TFT를 사용하고 있다. LTPS TFT는 높은 전자 이동도와 안정성을 가지고 있기 때문에 현재 각광 받는 AMOLED에 잘 맞는다. 하지만 LTPS TFT는 고비용, 250$^{\circ}C$ 이상의 공정온도, Substrate가 Glass, Metal로 제한 된다는 문제점이 있으며, 균일성이 낮고 현재 대면적 기술이 부족한 상태이다. 해결방안으로 AMOLED를 타겟으로 하는 Oxide TFT 기술이 떠오르고 있다. Oxide TFT는 이동도가 높고 저온공정이 가능하며 Substrate로 Plastic 기판을 사용할 수가 있어 차후에 Flexible 소자로서의 적용이 가능하다. 또한 기존의 진공장비 사용대신 용액공정이 가능하여 장비사용시간 및 절차를 단축시킬 수 있어 비용적인 유리함을 가지고 있다. Oxide TFT는 단결정 산화물과 다결정 복합 산화물 두 가지 범주를 가지고 있다. Oxide TFT의 재료물질은 ZnO, ZTO, IZO, SnO2, Ga2O3, IGO, In2O3, ITO, InGaO3(ZnO)5, a-IGZO이 있다. 본 연구에서는 산화물질 중 하나인 ZTO를 이용하여 TFT 소자를 제작하였다. 산화물 특성상 열처리 온도에 따라 형성되는 결정의 정도가 다르기 때문에 온도 및 시간 변수에 따른 ZTO의 특성변화에 초점을 맞추어 연구함으로서 최적화된 조건을 찾고자 실험을 진행하였다. 실험을 위한 기판으로 n-type wafer을 사용하였다. PE-CVD 장비를 이용하여 SiNx를 120 nm 증착하고, ZTO 용액을 spin-coating을 이용하여 channel layer을 형성하였다. 균일하게 형성된 ZTO의 결정을 위하여 200$^{\circ}C$, 300$^{\circ}C$, 400$^{\circ}C$, 500$^{\circ}C$에서 1시간, 3시간, 6시간, 10시간의 온도 및 시간 변수를 두어 공기 중에서 열처리 하였다. ZTO는 약 30 nm 두께로 형성되었다. Thermal evaporator를 이용하여 Source, Drain의 알루미늄 전극을 형성하고, wafer 뒷면에는 Silver paste를 이용하여 Gate전극을 만들었다. 제작된 소자를 dark room temperature에서 측정하였다.

• Journal of the Korean Applied Science and Technology
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• v.21 no.4
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• pp.345-351
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• 2004

Highly ordered pure-silica MCM-41 materials possessing well-defined morphology have been successfully prepared with surfactant used as a template. The fabrication of mesoporous silica has received considerable attention due to the need to develop more efficient materials' for catalysis, separations, and chemical sensing. The surface modified MCM-41 was used as anadsorbent for biomolecules. Silica-supported organic groups and DNA adsorption on surface modified MCM-41 were investigated by FT-IR and UV-Vis spectrometer, respectively. The use of MCM-41 as the modification of electrode surfaces were investigated electrochemical properties of metal mediators with biomolecules. The modified ITO electrodes increased peak currents for a redox process of $[Ru(bpy)_3]^{2+}$ relative to the bare electrode. The electrochemical detection of DNA by cyclic voltammetry when the current is saturated in the presence of the mediator appeared more sensitive due to a higher catalytic current on the MCM-41 supported electrodes modified by carboxylic acid functional groups. The carboxyl or amine groups on the surface of MCM-41 interact and react with the $-NH_2$ groups of guanine and backbone, respectively. Highly ordered mesoporous materials with organic groups could find applications as DNA sensors.

• Journal of the Korean Institute of Electrical and Electronic Material Engineers
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• v.29 no.3
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• pp.168-174
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• 2016

A conductive oxide-based sapphire glass indium tin oxide/metal electrode and the optical coating, through patterning process was studied in excellent optical properties and integrated touch panel has a high strength. Indium tin oxide conductive oxides of the sapphire glass to 0.3 A at DC magnetron sputtering method of 10 min, gas flow Ar 10 Sccm Ar, $O_2$ 1.0 Sccm the formation conditions of the thin film after annealing at $550^{\circ}C$ for 30min was achieved through a 86% transmittance. In addition, the coating 130 nm hollow silica sol-gel was to improve the optical transmittance of the indium tin oxide to 91%. For the measurement by the modeling hollow silica sol by Macleod simulation and calculated the average values of silica part to the presence or absence in analogy to actual. Refractive index value and the actual value of the material on the simulation the transmittance difference is it does not completely match the air region similar to the actual value (transmission) could be confirmed that the measurement is set to a value of between 5 nm and 10 nm.

• Journal of the Semiconductor & Display Technology
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• v.22 no.1
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• pp.23-27
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• 2023

Organic light-emitting diode(OLED) is very thin organic films which are hundreds of nanometers. Unlike bottom-emission OLED(BEOLED), top-emission OLED(TEOLED) emits light out the front, opaque moisture absorbents or metal foils can't be used to prevent moisture and oxygen. And it is difficult to have flexible characteristics with glass encapsulation, so thin film encapsulation which can compensate for those two disadvantages is mainly used. In this study, Al₂O₃ thin films by atomic layer deposition(ALD) were examined by changing the argon gas purge flow rate and we applied this Al₂O₃ thin films to the encapsulation of TEOLED. Ag / ITO / N,N'-Di-[(1-naphthyl)-N,N'-diphenyl]-1,1'-biphenyl-4,4'-diamine / tris-(8-hydroxyquinoline) aluminum/ LiF / Mg:Ag (1:9) were used to fabricate OLED device. The characteristics such as brightness, current density, and power efficiency are compared. And it was confirmed that with a thickness of 40 nm Al₂O₃ thin film encapsulation process did not affect OLED properties. And it was enough to maintain a proper OLED operation for about 9 hours.

• Journal of the Korean Vacuum Society
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• v.15 no.1
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• pp.64-72
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• 2006

We demonstrated organic light-emitting devices (OLEDs) based on the organic thin-film materials such as tris-(8-hydroxyquinoline) aluminum $(Alq_3)$. The structure of OLEDs was vacuum deposited upon transparent and thin glass substrates pre-coated with a transparent, conducting indium tin oxide thin film. The luminance characteristics, current, capacitance, and dispersion factor for degraded OLEDs, which were made by various bias currents $(0.5mA\;{\leq}\;I_{Bias}\;{\leq}9mA)$, are studied. The current dependences of lifetime were divided at approximately 2mA, and they represented nearly linear behaviors but had different slopes in a logarithmic plot of lifetime versus bias current. With lighting OLEDs, the anomaly of capacitance, as shown in the CV curve, occurred because of two factors, polarization in the bulk of organic materials and the interface between the metal and organic layers. In decayed OLEDs that had lower bias currents of less than 2mA, it was found that the degradation of luminance was related to both the decrease of polarization and to the lowering of the injection barrier.

• Electrical & Electronic Materials
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• v.12 no.7
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• pp.7-11
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• 1999

Fully sealed field emission display in size of 4.5 inch has been fabricated using single-wall carbon nanotubes-organic vehicle com-posite. The fabricated display were fully scalable at low temperature below 415$^{\circ}C$ and CNTs were vertically aligned using paste squeeze and surface rubbing techniques. The turn-on fields of 1V/${\mu}{\textrm}{m}$ and field emis-sion current of 1.5mA at 3V/${\mu}{\textrm}{m}$ (J=90${\mu}{\textrm}{m}$/$\textrm{cm}^2$)were observed. Brightness of 1800cd/$m^2$ at 3.7V/${\mu}{\textrm}{m}$ was observed on the entire area of 4.5-inch panel from the green phosphor-ITO glass. The fluctuation of the current was found to be about 7% over a 4.5-inch cath-ode area. This reliable result enables us to produce large area full-color flat panel dis-play in the near future. Carbon nanotubes (CNTs) have attracted much attention because of their unique elec-trical properties and their potential applica-tions [1, 2]. Large aspect ratio of CNTs together with high chemical stability. ther-mal conductivity, and high mechanical strength are advantageous for applications to the field emitter [3]. Several results have been reported on the field emissions from multi-walled nanotubes (MWNTs) and single-walled nanotubes (SWNTs) grown from arc discharge [4, 5]. De Heer et al. have reported the field emission from nan-otubes aligned by the suspension-filtering method. This approach is too difficult to be fully adopted in integration process. Recently, there have been efforts to make applications to field emission devices using nanotubes. Saito et al. demonstrated a car-bon nanotube-based lamp, which was oper-ated at high voltage (10KV) [8]. Aproto-type diode structure was tested by the size of 100mm $\times$ 10mm in vacuum chamber [9]. the difficulties arise from the arrangement of vertically aligned nanotubes after the growth. Recently vertically aligned carbon nanotubes have been synthesized using plasma-enhanced chemical vapor deposition(CVD) [6, 7]. Yet, control of a large area synthesis is still not easily accessible with such approaches. Here we report integra-tion processes of fully sealed 4.5-inch CNT-field emission displays (FEDs). Low turn-on voltage with high brightness, and stabili-ty clearly demonstrate the potential applica-bility of carbon nanotubes to full color dis-plays in near future. For flat panel display in a large area, car-bon nanotubes-based field emitters were fabricated by using nanotubes-organic vehi-cles. The purified SWNTs, which were syn-thesized by dc arc discharge, were dispersed in iso propyl alcohol, and then mixed with on organic binder. The paste of well-dis-persed carbon nanotubes was squeezed onto the metal-patterned sodalime glass throuhg the metal mesh of 20${\mu}{\textrm}{m}$ in size and subse-quently heat-treated in order to remove the organic binder. The insulating spacers in thickness of 200${\mu}{\textrm}{m}$ are inserted between the lower and upper glasses. The Y\ulcornerO\ulcornerS:Eu, ZnS:Cu, Al, and ZnS:Ag, Cl, phosphors are electrically deposited on the upper glass for red, green, and blue colors, respectively. The typical sizes of each phosphor are 2~3 micron. The assembled structure was sealed in an atmosphere of highly purified Ar gas by means of a glass frit. The display plate was evacuated down to the pressure level of 1$\times$10\ulcorner Torr. Three non-evaporable getters of Ti-Zr-V-Fe were activated during the final heat-exhausting procedure. Finally, the active area of 4.5-inch panel with fully sealed carbon nanotubes was pro-duced. Emission currents were character-ized by the DC-mode and pulse-modulating mode at the voltage up to 800 volts. The brightness of field emission was measured by the Luminance calorimeter (BM-7, Topcon).