• Journal of the Korean Crystal Growth and Crystal Technology
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• v.26 no.2
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• pp.74-79
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• 2016

The lanthanum oxide nano-rods were grown on the surface of 3 mol% Yttria Partially Stabilized Zirconia ceramic composite which containing Lanthanum-Strontium Manganate, $La_xSr_yMn_zO_3$ for the purpose of endorsing the antistatic property. The diameter and the aspect ratio of the nano-rods were greatly changed according to the growing condition. With the optical microscope observation, the nano-rods shining brightly. It was confirmed that the major components of nano-rods is La, and Sr, Mn, Si are minor components by SEM and TEM analyses.

• Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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• 2003.07b
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• pp.779-782
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• 2003

Hot filament 플라즈마 화학기상 증착법 (HFPECVD)를 사용하여 전처리 조건에 따른 탄소나노튜브의 성장 특성을 관찰하였다. 암모니아 ($NH_3$)를 희석가스로 사용하였고, 아세틸렌 ($C_2H_2$)를 탄소 원료가스로 각각 사용하였다. 암모니아 가스 플라즈마를 사용하여 전처리 된 니켈 촉매 층의 SEM (Scanning Electron Microscopy) 이미지를 관찰하여 본 결과, 나노 사이즈의 촉매 그레인(grain)을 발견할 수 있었다. 그리고 탄소 나노튜브의 직경과 성장 밀도 또한 전처리 된 촉매 층에 따라 다른 양상을 보였다. TEM (Transmission Electron Microscopy)를 사용하여 탄소나노튜브를 관찰한 결과 공동구조(hollow)를 한 다중벽 탄소 나노튜브(MWCNT)를 관찰할 수 있었다. 성장된 나노튜브는 끝에 금속팁을 가지고 있으며, 나노튜브의 팁은 촉매로 사용한 것과 같은 물질로 구성되어 있었다. Raman spectroscopy를 사용하여 측정된 B-밴드와 G-밴드의 피크들은 각각 $1360cm^{-1}$와 $1598cm^{-1}$ 부근에서 나타났으며, 전처리 조건을 달리하여 성장시킨 탄소나노튜브 필름에서 이들 두 피크의 위치는 이동하지 않았고, 두 피크의 강도 비율 ($I_G/I_D$)은 전처리 조건에 따라 변하였다.

• Proceedings of the Korean Vacuum Society Conference
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• 2014.02a
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• pp.220.1-220.1
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• 2014

본 연구에서는 PECVD 공법 중에 이온화 에너지가 높은 선형이온빔 소스를 이용하여 고온에서 전도성 카본박막을 코팅하였다. 카본 박막 코팅을 위한 Precursor는 $C_2H_2$ gas를 이용하였으며, 온도에 따른 카본 박막의 전기적 특성 및 두께에 따른 카본 박막 성장 구조를 분석하였다. 카본 박막의 전기적 특성은 Interfacial contact resistance (ICR) 방법으로 측정하였으며, 접촉 저항 측정을 위한 모재는 SUS316L stainless steel을 사용하였고 카본 박막 성장 구조 분석을 위해서는 폴리싱된 Si-wafer를 사용하였다. 선형이온빔 소스를 이용하여 상온에서 증착한 카본 코팅의 접촉저항 값은 50 nm 코팅 두께에서 $660m{\Omega}cm^2@10kgf/cm^2$으로 비정질상의 특성을 나타냈으며, 고온에서는 $14.8m{\Omega}cm^2@10kgf/cm^2$으로 온도가 증가함에 따라 비정질상의 카본 박막이 전도성을 가지는 카본박막으로의 성장을 확인할 수 있었다. 또한 전도성 카본 박막의 성장 구조 분석은 FE-SEM 및 Raman spectrum 분석을 통해 확인하였으며, 그 결과 코팅 두께가 증가할수록 카본 입자들은 수nm에서 약 150 nm의 카본 cluster를 형성하며 성장하였다. 이때 전도성 카본 박막의 두께에 따른 접촉저항의 값은 고온 조건에서 카본 박막의 두께가 약 100 nm일 때, $12.1m{\Omega}cm^2@10kgf/cm^2$의 가장 낮은 값을 가졌다. 위의 결과를 경제성이 아주 우수한 대면적 전도성 나노 카본 박막의 상용화 가능성이 높아질 것으로 기대된다.

• Transactions of the Korean Society of Mechanical Engineers A
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• v.36 no.7
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• pp.713-721
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• 2012

The finite element simulations of fatigue crack growth are carried out. Using only the mechanical properties usually obtained from the tensile test as input data, we attempted to predict the fatigue crack growth behavior. The critical crack opening displacement is determined by monitoring the change in displacements at the node close to the crack tip. Crack growth is simulated by debonding the crack tip node. The exponent in the Paris law was determined and compared to the published exponent. Plotting with respect to the effective stress intensity factor range yielded more consistent results.

• Proceedings of the Korean Vacuum Society Conference
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• 2011.02a
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• pp.445-445
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• 2011

본 연구에서는 편극 패턴된 강유전체 단결정 $LiNbO_3$ 기판에 광화학적 반응에 의해 금속(Au, Ag, Cu)나노입자를 표면에 선택적으로 성장하였다. 강유전체는 자발편극성의 특성을 지니고 있기 때문에 선택적으로 전압을 가하여 편극성의 역전에 의해 표면의 편극성을 선택적으로 패터닝이 가능하다. 본 연구에서는 주기적으로 양의 편극 영역과 음의 편극 영역이 패턴된 $LiNbO_3$ 기판을 사용하였다. 표면의 편극성은 압전소자반응현미경법(PFM)을 이용하여 확인하였으며, 극성은 R-V curve로 확인하였다. 금속입자는 금속입자를 포함하는 용액에 기판을 넣고 자외선을 조사하여 성장시켰다. 성장된 금속입자의 표면 분포 및 분석은 AFM을 이용하여 측정하였다. Ag 입자를 성장시킨 결과, (-z)편극 영역보다 (+z)편극영역에서 보다 많은 금속 나노입자들이 환원반응을 일으켜 나노입자를 형성하였으며, 경계영역 (inversion domain boundary)에 가장 많은 나노구조체가 형성되었다. Au 입자의 경우, (+z)편극영역이 (-z)편극영역의 표면보다 더 많은 입자가 형성되었지만 Ag입자처럼 편극영역의 경계에서 많이 증착되는 경향성은 보이지 않았다. Cu 입자의 경우 광화학반응을 거의 일으키지 않았으며, 편극영역에 따른 증착 경향성도 보이지 않았다. 이와 같은 결과를 증착된 금속 나노입자의 편극에 따른 표면분포를 강유전체 표면 극성에 따른 표면 밴드구조와, 각 입자가 지닌 환원전위와 전자친화도에 관련된 모델로 설명할 것이다.

• Korean Journal of Materials Research
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• v.6 no.6
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• pp.651-656
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• 1996

InGaAs/InGaAsP 다층박막을 corrugation이 형성된 InP 기판위에 MOVPE 방법을 이용하여 성장 시킨 후 성장조건에 따른 corrugation 높이의 변화와 석출상에 대하여 투과전자현미경을 이용하여 시킨 후 성장조건에 따른 corrugation 높이의 변화와 석출상에 대하여 투과전자현미경을 이용하여 연구하였다. Corrugation이 형성된 InP 기판을 PH3 및 AsH3가스를 동시에 공급해 주었는데 AsH3 가스의 압력이 높으면(1.8x10-2torr)많은 양의 As를 포함한 In1-xAsxP(x=0.3)석출상이 격자결함과 더불어 형성되었다. 반면에 AsH3 가스의 압력이 낮을때는 (1.0x10-3torr) corrugation의 높이가 30nm이었고, 적은 양의 As를 포함한 In1-xAsxP(x<0.1)석출상이 격자결함이 없이 형성되었다.

• Journal of Digital Convergence
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• v.17 no.2
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• pp.303-312
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• 2019

The purpose of this study was to describe the semantic system and process of posttraumatic growth experience of firefighters after colleague's suicide. Grounded theory methodology based on symbolic interactionism was utilized. The subjects of this study were 7 firefighters who experienced the colleague's suicide. Data were collected by using in-depth interviews from October 1 to November 30, 2015. The results showed that "Gradually becoming more resilient" was analyzed to be the core category of firefighters' posttraumatic growth. We derived four categories and nine subcategories. Based on the results, it is necessary to develop a convergence intervention program to promote posttraumatic growth of firefighters exposed to various traumatic events.

• Journal of the Korean Crystal Growth and Crystal Technology
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• v.23 no.6
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• pp.265-271
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• 2013

Czochralski (CZ) growth process is one of the most important techniques for growing high quality sapphire single crystal for LED application. In this study, the inductively-heated CZ growth processes for the sapphire crystal of 300 mm length have been analyzed numerically using finite element method. The hot zone structures were modified with the crucible geometry change and the additional insulation layer installed above the crucible. The results show that the solid-liquid interface height decreased from about 80 mm at initial stage to 40 mm after mid-stage due to achieve the growth speed balance. Also the optimal input power of the modified system was similar with the original one due to the compensation effects of the crucible geometry and additional insulation. The crystal temperature grown by the modified CZ grower was increased about 10 K than the original one. Therefore the sapphire crystal of 300 mm height was grown successfully.

• Journal of the Korean Vacuum Society
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• v.20 no.3
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• pp.211-216
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• 2011

In this study, the effects of growth temperature on structural and optical properties of hydrothermally grown ZnO nanorod arrays have been investigated. Zinc nitrate ($Zn(NO_3)_2$) and hexamethylenetetramine were used as precursors. The ZnO buffered Si(100) with a thickness of 40 nm was used as the substrates. The ZnO nanorods were grown on these substrates with the temperature ranging from 55 to $115^{\circ}C$. The results were characterized by scanning electron microscope, X-ray diffraction and room temperature photoluminescence measurements. Well-aligned ZnO nanorods arrays were obtained from all samples. The tips of nanorods were flat when the temperature was less than $95^{\circ}C$, and the sharp-tip nanoneedle-like morphologies were obtained with the temperature of $115^{\circ}C$. In addition, some bundles were on the nanorods arrays with $115^{\circ}C$ due to the non-equilibrium growth. The growth temperature could affect the crystal and optical properties of ZnO. For the effects on crystal properties, the intensity of (002) peak was increased as the temperature was increased to $75^{\circ}C$, then decreased as the temperature was further increased to $115^{\circ}C$. As for the effects on optical properties, the intensity ratio of UV peak to visible peak is increased with the temperature increasing and the strongest UV peak intensity was obtained with the growth temperature of $95^{\circ}C$.

• Clinical and Experimental Pediatrics
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• v.52 no.8
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• pp.922-929
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• 2009

Purpose : The aim was to investigate the clinical characteristics and responses to growth hormone (GH) therapy in children with attenuated growth who showed normal GH responses to GH stimulation tests (GHST). Methods : The study included 39 patients with height velocity (HV) of less than 4 cm/yr and normal GHST results. Clinical characteristics of patients were analyzed retrospectively. Results : Eleven were born as small for gestational age (SGA) and 28 as appropriate for age (AGA). In the SGA group, the standard deviation score (SDS) of age and height measured at their first visit was significantly low. Sixteen patients were treated with GH and six of 23 without GH therapy were followed for 1 year after GHST. The mean (range) of HV was 7.7 (4.9 to 11.1) cm/yr in patients with GH therapy and 3.7 (2.7 to 4.5) cm/yr in those without GH therapy, which was statistically significant (P<0.001). In the GH-treated group, HV and difference in height SDS during the treatment increased significantly (P<0.001; P< 0.001, respectively). HV increased after 1 year of GH therapy in the SGA and AGA groups (SGA, P=0.043; AGA, P=0.003). The level of Insulin-like growth factor-I was significantly lower in GH-treated patients with height SDS <-3 than those with ${\geq}3$ (P=0.023). Conclusion : In children with growth failure and normal GHST, HV increases significantly by short-term GH therapy. The assessment of long-term effects of GH therapy is necessary. Moreover, further studies should be considered to evaluate the GH-IGF-I axis due to the possibility of GH insensitivity syndrome.