• JSTS:Journal of Semiconductor Technology and Science
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• 제14권5호
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• pp.557-565
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• 2014

We report the effect of basal-plane stacking faults (BSFs) on X-ray diffraction (XRD) of non-polar (11$\underline{2}$0) a-plane GaN films with different $SiN_x$ interlayers. Complete $SiN_x$ coverage and increased three-dimensional (3D) to two-dimensional (2D) transition stages substantially reduce BSF density. It was revealed that the Si-doping profile in the Si-doped GaN layer was unaffected by the introduction of a $SiN_x$ interlayer. The smallest in-plane anisotropy of the (11$\underline{2}$0) XRD ${\omega}$-scan widths was found in the sample with multiple $SiN_x$ layers, and this finding can be attributed to the relatively isotropic GaN mosaic resulting from the increase in the 3D-2D growth step. Williamson-Hall (WH) analysis of the (h0$\underline{h}$0) series of diffractions was employed to determine the c-axis lateral coherence length (LCL) and to estimate the mosaic tilt. The c-axis LCLs obtained from WH analyses of the present study's representative a-plane GaN samples were well correlated with the BSF-related results from both the off-axis XRD ${\omega}$-scan and transmission electron microscopy (TEM). Based on WH and TEM analyses, the trends in BSF densities were very similar, even though the BSF densities extracted from LCLs indicated that the values were reduced by a factor of about twenty.

• 한국진공학회:학술대회논문집
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• 한국진공학회 2016년도 제50회 동계 정기학술대회 초록집
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• pp.247.1-247.1
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• 2016

Low-cost, high efficiency solar cells are tremendous interests for the realization of a renewable and clean energy source. ZnTe based solar cells have a possibility of high efficiency with formation of an intermediated energy band structure by impurity doping. In this work, ZnO/ZnTe:Cr and ZnO/i-ZnTe structures were fabricated by pulsed laser deposition (PLD) technique. A pulsed (10 Hz) Nd:YAG laser operating at a wavelength of 266 nm was used to produce a plasma plume from an ablated a ZnTe target, whose density of laser energy was 10 J/cm2. The base pressure of the chamber was kept at approximately $4{\times}10-7Torr$. ZnTe:Cr and i-ZnTe thin films with thickness of 210 nm were grown on p-Si substrate, respectively, and then ZnO thin films with thickness of 150 nm were grown on ZnTe:Cr layer under oxygen partial pressure of 3 mTorr. Growth temperature of all the films was set to $250^{\circ}C$. For fabricating ZnO/i-ZnTe and ZnO/ZnTe:Cr solar cells, indium metal and Ti/Au grid patterns were deposited on back and front side of the solar cells by using thermal evaporator, respectively. From the fabricated ZnO/ZnTe:Cr and ZnO/i-ZnTe solar cell, dark currents were measured by using Keithley 2600. Solar cell parameters were obtained under Air Mass 1.5 Global solar simulator with an irradiation intensity of 100 mW/cm2, and then the photoelectric conversion efficiency values of ZnO/ZnTe:Cr and ZnO/i-ZnTe solar cells were measured at 1.5 % and 0.3 %, respectively.

• 한국진공학회:학술대회논문집
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• 한국진공학회 2015년도 제49회 하계 정기학술대회 초록집
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• pp.197.2-197.2
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• 2015

Low-cost, high efficiency solar cells are tremendous interests for the realization of a renewable and clean energy source. ZnTe based solar cells have a possibility of high efficiency with formation of an intermediated energy band structure by impurity doping. In this work, the ZnTe:O/CdS/ZnO structure was fabricated by pulsed laser deposition (PLD) technique. A pulsed (10 Hz) Nd:YAG laser operating at a wavelength of 266 nm was used to produce a plasma plume from an ablated a ZnTe target, whose density of laser energy was 4.5 J/cm2. The base pressure of the chamber was kept at a pressure of approximately $4{\times}10-7Torr$. ZnO thin film with thickness of 100 nm was grown on to ITO/glass, and then CdS and ZnTe:O thin film were grown on ZnO thin film. Thickness of CdS and ZnTe:O were 50 nm and 500 nm, respectively. During deposition of ZnTe:O films, O2 gas was introduced from 1 to 20 mTorr. For fabricating ZnTe:O/CdS/ZnO solar cells, Au metal was deposited on the ITO film and ZnTe:O by thermal evaporation method. From the fabricated ZnTe:O/CdS/ZnO solar cell, current-voltage characteristics was measured by using HP 4156-a semiconductor parameter analyzer. Finally, solar cell performance was measured using an Air Mass 1.5 Global (AM 1.5 G) solar simulator with an irradiation intensity of 100 mW cm-2.

• 한국전기전자재료학회:학술대회논문집
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• 한국전기전자재료학회 2009년도 하계학술대회 논문집
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• pp.27-27
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• 2009

Non-stochiometric CdS:H films grown on polyethersulfon (PES) flexible polymer substrates at room temperature by R.F. sputtering technique. They exhibited a dark- and photo-sheet resistance of $2.7\times10^5$ and $\sim\;50\;{\Omega}$/square, respectively. These values were realized by an optimum control of both hydrogen doping-levels and the surface morphologies of the films. The comparison between the real and the simulated results for the shielding and the transmission by the free space measurement system in the X-band frequency range (8.2 - 12.4 GHz) was also addressed in this study. Samples overlapped with 13 layers of CdS:H/PES were consistent with the transmission results of pure aluminum metal films ($0.1\;{\Omega}$/square) deposited on PES substrates. As a result, by the simples tacking of the CdS:H/PES layers, the perfect control of the shielding and the transmission of the EM wave in the range of X-band frequency is possible by avisible light alone, and their results are especially very outstanding findings in the stealth function of the radome(Radar+Dome) such as aircrafts, ships, and missiles.

• 한국물환경학회지
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• 제32권1호
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• pp.46-51
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• 2016

In this study, we synthesized a combination of graphene oxide (GO) and titanium dioxide (TiO₂) and confirm that GO can be used for CO₂ photoreduction. TiO₂ exhibited highly efficient combination with other conventional electric charges generated by these paration phenomenon for suppression of hole-electron recombination. This improved the efficiency of CO₂ photoreduction. The synthetic form of GO-TiO₂ used in this study was agraphene sheet surrounded by TiO₂ powder. Efficiency and stability were enhanced by combination of GO and TiO₂. In a CO₂ photoreduction experiment, the highest CO conversion rate was 0.652 μmol/g·h in GO10-TiO₂ (2.3-fold that of pure TiO₂) and the highest CH₄ production rate was 0.037 μmol/g·h in GO0.1-TiO₂ (2.4-fold that of pure TiO₂). GO enhances photocatalytic efficiency by functioning as a support and absorbent, and enabling charge separation. With increasing GO concentration, the CH₄ level decreases to~45% due to decreased transfer of electrons. In this study, TiO₂ together with GO yielded a different result than the normal doping effect and selective CO₂ photoreduction.

• 한국결정성장학회지
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• 제4권3호
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• pp.325-335
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• 1994

Floating zone법으로 Spinel$(MgO.Al_2O_3)$을 성장시켰다. $MgO.Al_20_3$ spinel의 용융점은 $2135^{\circ}C$ 정도이고, 용융액으로부터 단결정을 성장시키는 방법에 있어서 매우 중용한 사항이다. Verneuil법과 RF-유도가열법을 이용한 czochralski법으로 성장시킨 경우가 보고된 바 있으나, 본 공법으로는 처음이라 사료된다. 본 연구에서는 halogen적외선 lamp를 이용한 image fur-nace에서 용융하여 아래쪽으로 하강함으로 인해 단결정을 육성시키는 floating zone법을 사용하여, $MgAl_2O_4$ spinel 단결정을 성장하였다. 또한 전이금속 이온을 doping하여 용융점의 하강 효과와 함께 적색, 녹색을 띈 단결정을 성장시켰다. 결론으로 성장계면과 용융대의 안전성에 주목하여 spinel 단결정 성장 기구를 규명하려 하였으며 성장계면이 오목함(결정쪽으로)에서 비롯되는 성장시의 양상에 대해 고찰하였다.

• 한국세라믹학회지
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• 제45권5호
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• pp.290-296
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• 2008

$AB'_{0.5}B"_{0.5}O_3$ type complex perovskite structures which have been reported as proton conductors over $600^{\circ}C$ were studied. The $AB'_{0.5}B"_{0.5}O_3$ type complex perovskite structure is known to be more easily synthesized and has better stability than normal $ABO_3$ perovskite structure. And it is stable at about $800^{\circ}C$ in the $CO_2$ atmosphere, whereas the $BaCeO_3$ perovskite is easily decomposed into carbonate. In addition, this $AB'_{0.5}B"_{0.5}O_3$ type complex perovskite structure could simply produce oxygen vacancies within their structure not by introducing additional doping oxides but by just controling the molar ratio of $B'^{+3}$ and $B"^{+5}$ metal ions in the B site. Hence it is easy to design the structure which shows highly sensitive electrical conductivity to humidity. In this study, the single phase boundary of $BaR_{0.5+x}Ta_{0.5-x}O_{3-{\delta}}$(R = rare earth) complex perovskite structures and it's phase stability were investigated with changes in composition, x. And the humidity dependance of electrical conductivity at different $P_{H2O}$ conditions was investigated.

• 한국자기학회지
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• 제15권3호
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• pp.181-185
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• 2005

반응성 스퍼터링 방법으로 성장시킨 $Zn_{0.09}Cr_{0.01}O$ 묽은 자성반도체 박막의 구조와 전기 수송과 자기 특성에 미치는 Al 첨가 효과를 탐구하였다. Al이 첨가되지 않은 $Zn_{0.09}Cr_{0.01}O$ 박막은 반도체적인 수송 특성과 함께 미약한 강자성 특성을 보였다. Al을 첨가함으로써 n-형 나르개인 전자의 농도 증가와 더불어 금속성 수송 특성을 나타냈으며 포화자기화가 현저하게 증가하고 이력곡선이 뚜렷하게 나타나는 등 자기 특성의 격렬한 변화가 관찰되었다. 이 결과들은 Cr이 첨가된 ZnO에서 나르개에 의한 강자성 질서의 향상을 보여준다.

• 한국진공학회:학술대회논문집
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• 한국진공학회 1999년도 제17회 학술발표회 논문개요집
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• pp.91-91
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• 1999

광소자 기술은 정보 전달 및 저장 기술의 지속적인 증가 요구에 따라 발전을 거듭하여 왔다. 특히 광통신 및 저장 기술에서 광원으로 사용되는 레이저 다이오드는 안정되면서 쉽게 제작할 수 있어야 한다. 이온 주입 방법은 반도체 공정에서 광범위하게 사용되는 공정이며 이미 소자측면에서 안정성이 확보되었다고 볼 수 있으나 대부분 메모리 등의 실리콘 반도체에서 이용되어 왔다. 최근에는 화합물 반도체 분야에서도 적용하는 예가 증가되고 있으나 광원으로 사용되는 레이저 다이오드의 경우는 우수한 품질의 반도체 층이 요구되며 따라서 damage가 큰 이온 주입 방법을 이용한 연구는 아직 많이 이루어져 있지 않다. 본 연구에서는 레이저 다이오드 구조의 성장측에 국부적으로 Fe 이온을 주입하여 도파로를 형성하여 광을 구속하여 도파시키는 동시에 전기적으로도 도파로 부분으로만 다이오드가 형성되도록 하고자 한다. 먼저 p층의 전기적 절연에 필요한 조건을 확보하기 위하여 CBE를 사용하여 Fe가 doping 된 SI-InP wafer 위에 p-InP (Be:5x1017 cm-3)층을 1.2$mu extrm{m}$ 성장한 후 ohmic 층으로 p-InGaAs (Be:1x1019 cm-3)을 0.1$\mu\textrm{m}$ 성장한 시료에 고에너지 이온 주입 장치를 사용하여 Fe 이온을 1MeV, 1.6meV의 에너지에 각각 1x1014cm-2, 2x1014cm-2 의 dose로 전면에 implant 하였다. 이 시료를 tube furnace에서 500, 600, $700^{\circ}C$각각 10분씩 annealing 한 후 재성장을 확인하기 위하여 DCXRD을 측정하였다. 그림 1은 DCXRD rocking curve로 annealing 하기 전 후의 In rich에서 side peak의 감소를 확인 할 수 있었는데 이는 damage가 어느 정도 복구되었음을 의미한다. 또한 절연 특성을 확인하기 위하여 ohmic metal을 증착하여 Hall 효과를 측정하였다. 그림 2에 보이는 것과 같이 annealing 온도가 증가함에 따라 면저항이 크게 증가함을 볼 수 있으며 이온 주입하기 전의 시료에 비해 104 이상의 저항을 갖을 수 있다. 향후 이러한 결과를 바탕으로 1.55$\mu\textrm{m}$ LD 구조에서 발진 특성을 관찰할 계획이다.

• 한국진공학회:학술대회논문집
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• 한국진공학회 2014년도 제46회 동계 정기학술대회 초록집
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• pp.193.1-193.1
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• 2014

This study was to investigate the electronic structure and optical properties of Na doped into NiO thin film using XPS and REELS. The films were grown by electron beam evaporation with varying the annealing temperature. The relationship between the electrical characteristics with the local structure of NiO thin films was also discussed. The x-ray photoelectron results showed that the Ni 2p spectra for all films consist of Ni 2p3/2 which indicate the presence of Ni-O bond from NiO phase and for the annealed film at temperature above $200^{\circ}C$ shows the coexist Ni oxide and Ni metal phase. The reflection electron energy loss spectroscopy spectra showed that the band gaps of the NiO thin films were slightly decreased with Na-doped into films. The Na-doped NiO showed relatively low resistivity compared to the undoped NiO thin films. In addition, the Na-doped NiO thin films deposited at room temperature showed the best properties, such as a p-type semiconducting with low electrical resistivity of $11.57{\Omega}.cm$ and high optical transmittance of ~80% in the visible light region. These results indicate that the Na doping followed by annealing process plays a crucial in enhancing the electrical and optical properties of NiO thin films. We believe that our results can be a good guide for those growing NiO thin films with the purpose of device applications, which require deposited at room temperature.