• 한국세라믹학회지
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• 제56권5호
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• pp.453-460
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• 2019

To reduce residual pores of composites and obtain a dense matrix, SiC_f/SiC composites were fabricated by chemical vapor deposition (CVI) using SiC nanorods. SiC nanorods were uniformly grown in the thickness direction of the composite preform when the reaction pressure was maintained at 50 torr or 100 torr at 1,100℃. When SiC nanorods were grown, the densities of the composites were 2.57 ~ 2.65 g/㎤, higher than that of the composite density of 2.47 g/㎤ for non-growing of SiC nanorods under the same conditions; grown nanorods had uniform microstructure with reduced large pores between bundles. The flexural strength, fracture toughness and thermal conductivity (room temperature) of the SiC nanorod grown composites were 412 ~ 432 MPa, 13.79 ~ 14.94 MPa·m^1/2 and 11.51 ~11.89 W/m·K, which were increases of 30%, 25%, and 25% compared to the untreated composite, respectively.

• 한국재료학회:학술대회논문집
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• 한국재료학회 2003년도 춘계학술발표강연 및 논문개요집
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• pp.173-173
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• 2003

• 한국재료학회:학술대회논문집
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• 한국재료학회 2003년도 춘계학술발표강연 및 논문개요집
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• pp.172-172
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• 2003

• 한국진공학회:학술대회논문집
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• 한국진공학회 2009년도 제38회 동계학술대회 초록집
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• pp.189-189
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• 2010

ZnO nanorods 구조는 광소자 및 태양광 소자의 성능을 향상시키기 위해서 무반사계수, 광추출효율, 전기적, 열적 전도도를 개선시킬 수 있어, 매우 큰 관심을 가지고 왔다. 또한 Ag 나노입자는 표면 플라즈몬 효과를 이용하여 LED나 태양전지에 응용하여 소자의 성능이 향상됨을 이론적, 실험적으로 증명되어 왔으며, 현재에도 활발한 연구가 진행되고 있다. 이러한 ZnO nanorods 특성과 Ag 나노입자의 표면 플라즈몬 효과를 이용하기 위해서, 본 연구에서는 Ag 나노 입자를 형성된 ZnO seed층에 ZnO nanorods를 성장시켰다. 시료를 제작을 위해서 비교적 성장이 간단하고 저온성장이 가능한 화학적 합성방법을 이용하였다. Ag 나노입자가 형성된 ZnO seed층 제작을 위해서 먼저 Si 기판위에 RF magnetron 스퍼터를 이용하여 고진공, $N_2$ 분위기에서 일정한 두께로 증착을 하였으며, 이후 Ag 박막을 thermal evaporator로 10 nm 두께로 증착하였다. 그 다음, 크기가 다른 Ag 나노입자를 형성을 위해서 rapid thermal annealing (RTA)을 여러 가지 온도에서 수행하였다. 그리고 이러한 시료들를 이용하여, ZnO nanorods를 성장하기 위하여, $90-95^{\circ}$의 온도에서 zinc nitrate $Zn(NO_3)_2{\cdot}6H_2O$과 hexamethylentetramines (HMT)으로 혼합된 용액에 담가두어 ZnO nanorods를 성장시켰다. Ag 나노입자의 크기에 따라 ZnO nanorods의 구조와 형태에 대하여 어떠한 영향을 주는지를 관찰하기 위해 field emission scanning electron microscopy (FE-SEM)을 이용하여 측정하였으며, Ag와 ZnO의 성분분석과 결정성을 조사하기 위해 X-ray diffraction (XRD)을 이용하여 분석하였다. 그리고 표면 플라즈몬에 의한 영향에 대하여 조사하기 위해, ZnO nanorods와 Ag 나노입자가 형성된 ZnO nanorods를 UV-Vis-NIR spectrophotometer을 이용하여 흡수계수와 반사계수를 비교하여 측정하였으며. 태양전지의 성능향상을 수 있음을 이론적으로 계산하였다. 그리고 또한 photoluminescence (PL) 분석을 수행하여 ZnO nanorods의 구조에 대하여 Ag 나노입자의 영향에 대한 광특성을 측정하였다.

• 한국진공학회:학술대회논문집
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• 한국진공학회 2013년도 제44회 동계 정기학술대회 초록집
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• pp.349-349
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• 2013

질화물 기반 물질은 발광다이오드의 효율 향상과 함께 널리 연구되는 물질의 하나이다. 그러나, 고유의 물성적 특성으로 인한 압전전기장 효과는 넓은 가시광영역에서 궁극적 효율 달성을 위한 장애가 되고 있다. 이를 극복하기 위한 방법 중 하나는 나노 구조이며, 특히 비극성면을 통한 나노구조의 구현은 압전전기장 효과를 제거할 수 있는 장점이 있다. 그러나, 현재까지 이를 위한 질화물 나노로드의 구현은 보통의 경우 발생하는 반극성면의 발현으로 인해 기술적 어려움이 많았다. 이를 위해 제시되는 방법 중 하나인 반복적 성장 기법을 통한 본 그룹의 성공적 나노로드의 구현과 함께, nucleation 조건의 변화에 따른 성장 과정을 분석하여 미래의 고효율 3차원 나노구조 발광 소자를 위한 단서를 제공하고자 한다. Fig. 1은 수소(a)와 질소(b)를 850도부터 1,050도까지 성장 온도를 달리하여 성장했을 때의 모양 변화를 나타내며 이를 통한 GaN nanorod 성장 영향에 대하여 논하고자 한다.

• 한국재료학회지
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• 제22권4호
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• pp.180-184
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• 2012

Nanostructures of ZnO, such as nanowires, nanorods, nanorings, and nanobelts have been actively studied and applied in electronic or optical devices owing to the increased surface to volume ratio and quantum confinement that they provide. ZnO seed layer (about 40 nm thick) was deposited on Si(100) substrate by RF magnetron sputtering with power of 60 W for 5 min. ZnO nanorods were grown on ZnO seed layer/Si(100) substrate at $95^{\circ}C$ for 5 hr by hydrothermal method with concentrations of $Zn(NO_3)_2{\cdot}6H_2O$ [ZNH] and $(CH_2)_6N_4$ [HMT] precursors ranging from 0.02M to 0.1M. We observed the microstructure, crystal structure, and photoluminescence of the nanorods. The ZnO nanorods grew with hexahedron shape to the c-axis at (002), and increased their diameter and length with the increase of precursor concentration. In 0.06 M and 0.08 M precursors, the mean aspect ratio values of ZnO nanorods were 6.8 and 6.5; also, ZnO nanorods had good crystal quality. Near band edge emission (NBE) and a deep level emission (DLE) were observed in all ZnO nanorod samples. The highest peak of NBE and the lower DLE appeared in 0.06 M precursor; however, the highest peak of DLE and the lower peak of NBE appeared in the 0.02 M precursor. It is possible to explain these phenomena as results of the better crystal quality and homogeneous shape of the nanorods in the precursor solution of 0.06 M, and as resulting from the bed crystal quality and the formation of Zn vacancies in the nanorods due to the lack of $Zn^{++}$ in the 0.02 M precursor.

• 한국전기전자재료학회논문지
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• 제16권6호
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• pp.454-459
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• 2003

We investigate the structure and properties of SiC (Silicon Carbide) nanotubes using molecular dynamics simulation based on the Tersoff bond-order potential. For small diameter tubes, the Si-C bond distance of SiC nanotubes decreases as the nanotube diameter is decreased, due to curvature of the nanotube surface. We find that Young's modulus of SiC nanotubes is somewhat smaller than that of the other nanotubes considered so far. However, Young's modulus for SiC nanotubes is larger than that of ${\beta}$-SiC and almost equal to the experimental value for SiC nanorod and SiC whisker. The strain energy of the SiC nanotubes is also lower than that of the other nanotubes. The lower strain energy of SiC nanotubes raises the possibility of synthesis of SiC nanotubes.

• 한국분말재료학회지
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• 제22권6호
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• pp.391-395
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• 2015

We report on the successful fabrication of ZnO nanorod (NR)/polystyrene (PS) nanosphere hybrid nanostructure by combining drop coating and hydrothermal methods. Especially, by adopting an atomic layer deposition method for seed layer formation, very uniform ZnO NR structure is grown on the complicated PS surfaces. By using zinc nitrate hexahydrate $[Zn(NO_3)_2{\cdot}6H_2O]$ and hexamine $[(CH_2)_6N_4]$ as sources for Zn and O in hydrothermal process, hexagonal shaped single crystal ZnO NRs are synthesized without dissolution of PS in hydrothermal solution. X-ray diffraction results show that the ZnO NRs are grown along c-axis with single crystalline structure and there is no trace of impurities or unintentionally formed intermetallic compounds. Photoluminescence spectrum measured at room temperature for the ZnO NRs on flat Si and PS show typical two emission bands, which are corresponding to the band-edge and deep level emissions in ZnO crystal. Based on these structural and optical investigations, we confirm that the ZnO NRs can be grown well even on the complicated PS surface morphology to form the chestnut-shaped hybrid nanostructures for the energy generation and storage applications.

• 대한금속재료학회지
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• 제49권5호
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• pp.400-405
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• 2011

ZnO nanotube arrays were synthesized by a two-step process: electrodeposition and selective dissolution. In the first step, ZnO nanorod arrays were grown on an Au/Si substrate by using a homemade electrodeposition system. ZnO nanorod arrays were then selectively dissolved in an etching solution composed of 0.125 M NaOH, resulting in hollow ZnO nanotube arrays. It is suggested that the formation mechanism of the ZnO nanotube arrays might be attributed to the preferred surface adsorption of hydroxide ion ($OH^{-1}$) on a positive polar surface followed by selective dissolution of the metastable Zn-terminated ZnO (0001) polar surface caused by the difference in the surface energy per unit area between the ZnO nanorod and nanotube.

• 한국진공학회:학술대회논문집
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• 한국진공학회 2014년도 제46회 동계 정기학술대회 초록집
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• pp.421.2-421.2
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• 2014

We report on the growth of ZnO nanorods (NRs) grown on graphite and silicon substrates via an all-solution process and characteristics of their heterojunctions. Structural investigations indicated that morphological and crystalline properties were not significantly different for the ZnO NRs on both substrates. However, optical properties from photoluminescence spectra showed that the ZnO NRs on graphite substrate contained more point defects than that on Si substrate. The ZnO NRs on both substrates showed typical rectification properties exhibiting successful diode formation. The heterojunction between the ZnO NRs and the graphite substrate showed a Schottky diode characteristic and photoresponse under ultraviolet illumination at a small reverse bias of -0.1 V. The results showed that the graphite substrate could be a good candidate for a Schottky contact electrode as well as a conducting substrate for electronic and optoelectronic applications of ZnO NRs.