• Journal of the Korean Ceramic Society
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• v.30 no.5
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• pp.404-410
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• 1993

The characterization and sintering behavior of ZnO powders prepared by precipitation method were investigated. ZnO powders were synthesized using the aqueous solutions of ZnCl2 and NH4OH as a precipitation agent, which were crystallized in the shape of plate-like. The grain growth of ZnO(0.68${\mu}{\textrm}{m}$, 1.3${\mu}{\textrm}{m}$ and 3.4${\mu}{\textrm}{m}$) has been studied for temepratures from 100$0^{\circ}C$ to 130$0^{\circ}C$, and the rate of densification was inversely proportional to the ZnO particle size. Densification proceeded slowly by diffusion mechanisms above at 100$0^{\circ}C$. In this work, the grain growth kinetic exponent(n) was 3. The temperature dependence of ZnO grain growth was plotted, and the activation energy of grain growth was 75~85Kcal/mol.

• Proceedings of the Korean Vacuum Society Conference
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• 2013.08a
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• pp.209.2-209.2
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• 2013

We proposed and fabricated zinc oxide thin-film transistors (TFTs) employing 4-mercaptophenol (4MP) doped ZnO by atomic layer deposition (ALD) that results in highly stable and high performance. The 4MP concentration in ZnO films were varied from 1.7% to 5.6% by controlling Zn:4MP pulses. The n-type carrier concentrations in ZnO thin films were controlled from $1.017{\times}10^{20}/cm^3$ to $2.903{\times}10^{17}/cm^3$ with appropriate amount of 4MP doping. The 4.8% 4MP doped ZnO TFT revealed good device mobility performance of 8.4 $cm^2/Vs$ and the on/off current ratio of 106. Such 4MP doped ZnO TFTs exhibited relatively good stability (${\Delta}V_{th}$: 2.4 V) under positive bias-temperature stress while the TFTs with only ZnO showed a 4.3 ${\Delta}V_{th}$ shift, respectively.

• Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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• 2006.11a
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• pp.145-146
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• 2006

The most Important research topic in the development of ZnO LED and LD is the production of p-type ZnO thin film that has minimal stress with outstanding stoichiometric ratio. In this study, Phosphorus diffused into the undoped ZnO thin films using the ampoule-tube method for the production of p-type znO thin films. The undoped ZnO thin films were deposited by RF magnetron sputtering system on $GaAs_{0.6}P_{0.4}$/GaP and Si wafers. 4N Phosphorus (P) was diffused into the undoped ZnO thin films in ampoule-tube which was performed and $630^{\circ}C$ during 3hr. We found the diffusion condition of the conductive ZnO films which had p-type properties with the highest mobility of above 532 $cm^2$/Vs compared with other studies PL spectra measured at 10K for the purpose of analyzing optical properties of p-type ZnO thin film showed strong PL intensity in the UV emission band around 365nm ~ 415nm and 365nm ~ 385nm.

• Proceedings of the Korean Vacuum Society Conference
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• 2013.08a
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• pp.208-208
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• 2013

ZnO는 직접천이형 반도체로 약 3.37 eV의 넓은 에너지 band-gap과 60 meV의 비교적 큰 엑시톤 결합 에너지를 가지고 있다. 또한 단결정 성장 가능과 투명성 등 많은 장점들로 인하여 GaN와 대체할 자외선 또는 청색 발광소자나 ITO를 대체할 투명전극 같은 광범위한 광전소자로 큰 주목을 받으며 연구되어 왔다. 이러한 ZnO는 다양한 물질들의 첨가를 통해 인위적으로 특성변화가 가능한데 Mg, Be, Cd 첨가를 통한 에너지 밴드갭의 확장과 수축, Al 첨가를 통한 전기전도성의 증가 등이 그 예이다. 최근에는 밴드갭 조절을 이용한 ZnO-ZnMgO와 같은 이종접합구조가 광소자 등의 응용을 목적으로 많은 연구가 이루어지고 있다. 더불어 나노선이나 나노막대 같은 1차원 구조를 갖는 ZnO 계열 반도체의 연구는 현재 큰 이슈가 되고 있는 나노 크기의 소자 개발에 매우 큰 적용 가능성을 가지고 있다. 우리는 수열합성법을 이용하여 hexagonal ZnO 나노막대를 성장하고 그 표면에 core-shell 형태의 $ZnO-Zn_{1-x}Mg_xO$ (x=0.084) 양자우물을 원자층증착법으로 증착하였다. 본 연구에서는 만들어진 ZnO 나노막대와 ZnO-ZnMgO 나노막대, core-shell ZnO-ZnMgO 양자우물 sample들의 저온(5 K) Photoluminescence 측정을 통하여 광학적 band 구조를 분석하였다. 실험적으로 의도된 양자우물 두께와 다른 실제 형성된 양자무물의 두께를 알아내기 위하여 2차원 hexagonal 양자우물 band 구조에서 self-consistent nonlinear Poisson-Schr$\"{o}$dinger 방정식 계산과 컴퓨터 시뮬레이션을 이용하였으며, 이 방법으로 계산된 값과 실험값의 비교를 통하여 실제 형성된 양자우물의 두께를 정량적으로 유출할 수 있었다.

• Journal of the Korean Ceramic Society
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• v.41 no.1
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• pp.76-80
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• 2004

Nano-sized ZnO colloids were prepared by use of spray combustion method. for combustion reaction, $Zn(NO_3)_2{\cdot}6H_2O$ and $CH_6N_4O$ were employed as an oxidizer and a fuel. Exothermic peak was shown at $230^{\circ}C$ by DTA/TGA, and it was considered as a combustion reaction followed by ignition of the precursor mixture. In case of spray combustion method, because insufficient contents of molecules and radicals generated from precursor droplets may lead an incomplete igmition, the ignition temperature of combustion chamber was chosen at $500^{\circ}C$. For diminishing aerosol coagulation, the droplet number concentration was reduced by filter media. The fluid was laminar with 2.5 seconds of aerosol residence time. The synthesized colloids had spherical shape with 180 nanometer size, and the crystalline phase was ZnO with hexagonal structure.

• Korean Journal of Materials Research
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• v.13 no.6
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• pp.347-351
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• 2003

II-Ⅵ ZnO compound semiconductor thin films were grown on $\alpha$-Al$_2$O$_3$(0001) single crystal substrate by radical beam assisted molecular beam epitaxy and the optical properties were investigated. Zn(6N) was evaporated using Knudsen cell and O radical was assisted at the partial pressure of 1$\times$10$^{4}$ Torr and radical beam source of 250-450 W RF power. In $\theta$-2$\theta$ x-ray diffraction analysis, ZnO thin film with 500 nm thickness showed only ZnO(0002)and ZnO(0004) peaks is believed to be well grown along c-axis orientation. Photoluminescence (PL) measurement using He-Cd ($\lambda$=325 nm) laser is obtained in the temperature range of 9 K-300 K. At 9 K and 300 K, only near band edge (NBE) is observed and the FWHM's of PL peak of the ZnO deposited at 450 RF power are 45 meV and 145 meV respectively. From no observation of any weak deep level peak even at room temperature PL, the ZnO grains are regarded to contain very low defect density and impurity to cause the deep-level defects. The peak position of free exciton showed slightly red-shift as temperature was increased, and from this result the binding energy of free exciton can be experimentally determined as much as $58\pm$0.5 meV, which is very closed to that of ZnO bulk. By van der Pauw 4-point probe measurement, the grown ZnO is proved to be n-type with the electron concentration($n_{e}$ ) $1.69$\times$10^{18}$$cm^3$, mobility($\mu$) $-12.3\textrm{cm}^2$/Vㆍs, and resistivity($\rho$) 0.30 $\Omega$$\cdot$cm.

• Electrical & Electronic Materials
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• v.9 no.7
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• pp.708-718
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• 1996

The microstructure and electrical properties of the nonlinear ZnO varistor with A1$_{2}$ $O_{3}$ additions is investigated. The variation of nonlinear behavior with A1$_{2}$ $O_{3}$ additions is indicated from J-E and C-V measurement to be a result of the change of the interface defects density $N_{t}$ at the grain boundaries and the donor concentration $N_{d}$ in the ZnO grains. The optimum composition which has the nonlinear coefficients of -57 was observed in the sample with 0.005wt% A1$_{2}$ $O_{3}$ additions. The conduction mechanism at the pre-breakdown region is consistent with a Schottky thermal emission process obeying a relation given by $J^{\var}$exp[-(.psi.-.betha. $E^{1}$2/)kT] and the conduction process at the breakdown region follows a Fowler-Nordheim tunneling mechanism of the form $J^{\var}$exp(-.gamma./E).

• Proceedings of the Korean Vacuum Society Conference
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• 2010.08a
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• pp.164-164
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• 2010

The impurity doped ZnO has been extensively studied because of its optoelectric properties. GIZO (Ga-In-Zn-O) amorphous oxide semiconductors has been widely used as transparent flexible semiconductor material. Recently, various amorphous transparent semiconductors such as IZO (In-Zn-O), GIZO, and HIZO (Hf-In-Zn-O) were developed. In this work, we examined the local structures of IZO, GIZO, and HIZO. The local coordination structure was investigated by the extended X-ray absorption fine structure. The IZO, GIZO and HIZO thin films ware deposited on the glass substrate with thickness of 400nm by the radio frequency sputtering method. The targets were prepared by the mixture of $In_2O_3$, ZnO and $HfO_2$ powders. The percent ratio of In:Zn in IZO, Ga:In:Zn in GIZO and Hf:In:Zn in HIZO was 45:55, 33:33:33 and 10:35:55, respectively. In this work, we found that IZO, GIZO and HIZO are all amorphous and have a similar local structure. Also, we obtained the bond distances of $d_{Ga-O}=1.85\;{\AA}$, $d_{Zn-O}=1.98\;{\AA}$, $d_{Hf-O}=2.08\;{\AA}$, $d_{In-O}=2.13\;{\AA}$.

• Proceedings of the Materials Research Society of Korea Conference
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• 2003.03a
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• pp.95-95
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• 2003

최근, 대면적 평판표시소자 제작을 위한 전기발광 (EL; electroluminescence)소자용 소재로서 GaN 분말을 적용하고자 하는 연구가 진행되고 있다. 이와 같이 GaN 분말을 EL 소재로 사용하기 위해서는 원하는 파장의 빛을 발광할 수 있도록 특정의 불순물을 첨가하여야 할 필요가 있다. Mg이 첨가된 GaN 분말의 합성과 특성에 대한 연구가 있었으며, 희토류 원소가 첨가된 GaN 분말의 특성이 보고된바 있다. 본 논문에서는 GaOOH 분말을 출발물질로 채택하여 Zn가 첨가된 GaN 분말을 합성하고 광학적인 특성을 조사하였다. Zn가 첨가된 GaN 분말을 합성하기 위하여, 우선 CaOOH 분말 1g과 일정량의 ZnO 또는 Zn(NO$_3$)$_3$를 함께 섞어 유발에서 습식 혼합한 후 건조시켰다. Ga에 대한 Zn의 몰 비는 0.1부터 30 까지 변화시켰다. 반응온도는 900~110$0^{\circ}C$의 범위에서 변화시켰고, 반응시간은 1~4시간 범위에서 변화시켰으며, NH$_3$의 유량은 400 sccm으로 하였다. X선 회절분석장치를 사용하여 결정구조를 확인하였고, Zn의 첨가에 따른 광학적 특성은 10 K의 온도에서 광루미네센스(PL; photoluminescence)를 측정하여 평가하였다.

• Proceedings of the Materials Research Society of Korea Conference
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• 2011.05a
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• pp.24-24
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• 2011

ZnO 직접 천이형의 와이드밴드갭 화합물 반도체로써 높은 엑시톤 결합 에너지를 가짐으로 해서 광전자나 광학디바이스로의 넓은 응용범위를 갖고 있다. 최근들어 ZnO의 비선형 광학 특성이 보고 됨으로써 새로운 광학 재료로서의 연구도 기대되고 있다. 본연구에서는 새로운 주기적 반전 구조를 제안함으로 해서 극성을 가지는 화합물 반도체의 비선형 광학 디바이스로의 응용 범위를 넓히고자 한다. ZnO는 Wurtzite 구조를 가짐으로 해서 성장 방향으로 Zn-극성 및 O-극성을 가지게 된다. 이런 자연 발생적인 극성에 의해 물리적, 화학적, 광학적 특성들이 바뀌게 됨으로, 극성의 제어는 재료의 특성을 극대화 시키기 위해 아주 중요한 항목이 되어 있습니다. 본 연구에서는 손쉽고 재현성이 확보되는 방법으로써, CrN 와 Cr2O 3의 완충층을 제안하여 ZnO 극성의 제어를 이루었고, 제안된 극성 제어 방식을 이용하여 주기적으로 Zn-극성과 O-극성이 배열된 구조(PPI 구조)를 형성 하였다. 패터닝과 재성장 방법을 통해서 다양한 구조와 사이즈의 1D, 2D PPI ZnO를 제작하는데 성공하였다. 주기적인 반전구조의 제작을 확인하기 위해 PRM(piezo response miscosocpy)이라는 방법을 통하여 주기적 극성 선택성을 확인하였으며, TEM과 PL 분석법을 통하여 구조적 광학적 특성을 분석하였다. 새롭게 제안된 극성 제어 방식을 이용하여 제작된 PPI 구조를 이용하여 비선형 광학소자로의 응용성을 확인하였다. 본발표에서는 PPI ZnO 구조의 형성방법, 분석 및 응용에 대한 제안과 결과가 논의될 것이다.