• Corrosion Science and Technology
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• 제18권6호
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• pp.267-276
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• 2019

The purpose of this study was to examine the influence of conditions for quenching and/or tempering on the corrosion and hydrogen diffusion behavior of ultra-strong automotive steel in terms of the localized plastic strain related to the dislocation density, and the precipitation of iron carbide. In this study, a range of analytical and experimental methods were deployed, such as field emission-scanning electron microscopy, electron back scatter diffraction, electrochemical permeation technique, slow-strain rate test (SSRT), and electrochemical polarization test. The results showed that the hydrogen diffusion parameters involving the diffusion kinetics and hydrogen solubility, obtained from the permeation experiment, could not be directly indicative of the resistance to hydrogen embrittlement (HE) occurring under the condition with low hydrogen concentration. The SSRT results showed that the partitioning process, leading to decrease in localized plastic strain and dislocation density in the sample, results in a high resistance to HE-induced by aqueous corrosion. Conversely, coarse iron carbide, precipitated during heat treatment, weakened the long-term corrosion resistance. This can also be a controlling factor for the development of ultra-strong steel with superior corrosion and HE resistance.

• 한국진공학회:학술대회논문집
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• 한국진공학회 2015년도 제49회 하계 정기학술대회 초록집
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• pp.120.2-120.2
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• 2015

We propose a novel direct writing technique with a femtosecond laser enabling selective modification of not only the morphology of conducting polymer thin films but also the orientation and alignment of the polymer crystal. Surface relief gratings resulting from photoexpansion on P3HT:PCBM and PEDOT:PSS thin films were fabricated by femtosecond laser direct writing. The photoexpansion was induced at laser fluence below the ablation threshold of the thin film. The morphology (size and shape) of photoexpansion could be quantitatively controlled by laser writing parameters such as focused beam size, writing speed, and laser fluence. GIWAX results showed that face-on P3HT crystals were largely increased in the photoexpansion in comparison with pristine region of the thin film. In addition, the face-on P3HTs in the photoexpansion were aligned with their orientation along the polarization of the laser. The micro-RAMAN spectra confirmed that neither chemical composition change nor the polymer chain breaking was observable after femtosecond laser irradiation. We believe that this laser direct writing technique opens a new door to the fabrication of more efficient OPVs via non-contact, toxic-free approach.

• Transactions on Electrical and Electronic Materials
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• 제12권2호
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• pp.64-67
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• 2011

The effect of Ta substitution on the crystal structure, ferroelectric, and piezoelectric properties of $Bi_{0.5}(Na_{0.82}K_{0.18})_{0.5}Ti_{1-x}Ta_xO_3$ ceramics has been investigated. The Ta doping resulted in a transition from coexistence of ferroelectric tetragonal and rhombohedral phases to an electrostrictive pseudocubic phase, leading to degradations of the remnant polarization, coercive field, and piezoelectric coefficient $d_{33}$. However, the electricfield-induced strain was significantly enhanced by the Ta substitution-induced phase transition and reached a highest value of $S_{max}/E_{max}$ = 566 pm/V under an applied electric field 6 kV/mm when 2% Ta was substituted on Ti sites. The abnormal enhancement in strain was attributed to the pseudocubic phase with high electrostrictive constants.

• 한국전기전자재료학회논문지
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• 제14권7호
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• pp.562-566
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• 2001

The effects of MnO$_2$ addition on the properties in Pb(Mg$_{1}$3/Nb$_{2}$3/)O$_3$ relaxor ferroelectrics were studied in the phase transition temperature range from -4$0^{\circ}C$ to 11$0^{\circ}C$. Specimens were made via solid state processing method. Dielectric properties, piezoelctric properties, electric-field-induced strain were examined to clarify the effect of MnO$_2$ addition in 0.9MN-0.1PT. As the amount of MnO$_2$ increases, the maximum dielectric constant and the dielectric loss decreases. Q$_{m}$ increased by increasing the doping contents of Mn. When 0.5wt% MnO$_2$ was doped, Q$_{m}$ increased from 95 to 480. The electric-filed-induced strain and polarization decreases as the amount of MnO$_2$ increases. From the experimental results, it was suggested that Mn behaves as an ferroelectric domain pinning element.ent.

• Journal of the Optical Society of Korea
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• 제8권1호
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• pp.6-12
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• 2004

Diffraction Bragg gratings consisting of metal (silver) nanoparticles are generated inside a soda-lime glass substrate. After ion-exchanging and annealing processes in the glass, the silver nanoparticles are first formed with the particle diameters of 10 nm ∼ 30 nm. By interfering two CW laser beams at ∼ 60 ${\mu}{\textrm}{m}$ deep under the surface of the nanoparticles-dispersed glass, Bragg gratings with thickness of 15 ${\mu}{\textrm}{m}$ and period of 3.5 ${\mu}{\textrm}{m}$ are generated. Diffraction efficiency of the gratings formed by two TE-polarized beams is three times higher than that by two TM-polarized beams. From this polarization dependence, we have found that strong coupling of the surface plasmons induced on the metal particles may contribute dominantly to generate the diffraction grating.

• 한국전자파학회지:전자파기술
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• 제6권1호
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• pp.10-16
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• 1995

완전도체 스트립 회절격자에 의한 E-분극 산문제를 모멘트법을 이용하여 해석하였다. E분극의 경우는 청도 되는 표면전류밀도가 모서리 양 끝에서 매우 높을 것으로 추측된다. 이때 스트립에 청도되는 표면전류밀도는 차수가 0인 Ultraspherical 다항식의 급수와 적절한 모서리 경계조건을 만족하는 함수의 곱의 급수로 전개하였다. 전류밀도와 반사계수에 대한수직결과를 기존의 다른 수틀과 비교하였다. 본 논문의 수치결과가 기존의 다른 수를 사용했을 때 보다 기하학적 반사계수의 경도가 매우 빠르게 향상됨을 보였다. 기하학적 반사계수에서의 급변점 위치는 입사각, 스트립 폭 및 스트립 주기를 변화시킴으로써 이동시킬 수 있었다.

• Bulletin of the Korean Chemical Society
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• 제19권8호
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• pp.847-851
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• 1998

13C, 15N, and 29Si NMR chemical shifts have been computed for selected X-substituted silatranes (X=Cl, F, H, CH3) using Gauge-Including Atomic Orbitals (GIAO) and Continuous Set of Gauge Transformations (CSGT) at the Hartree-Fock level of theory. The isotropic 13C chemical shifts are largely insensitive to substituent-induced structural changes. In this study, the isotropic 13C chemical shifts GIAO and CSGT calculations at the HF/6-31G and HF/6-31G* levels are sufficiently accurate to aid in experimental peak assignments. The isotropic 13C chemical shifts X-substituted silatranes at HF/6-31G* level are approximately 4 ppm different from the experimental values. In contrast, the isotropic 15N and 29Si chemical shifts and the chemical shielding tensors are quite sensitive to substituent-induced structural changes. These trends are consistent with those of the experiment. The 15N chemical shift parameters demonstrate a very clear correlation with Si-N distance, especially when we use the polarization function. Changes in anisotropy, 3a as well as in the 15N isotropic chemical shifts are due primarily to changes in the value of a.. But in case of "Si the correlations are not as clean as for the 15N chemical shift.

• BioChip Journal
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• 제12권4호
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• pp.317-325
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• 2018

This paper investigated the effects of ionic strength in the medium on a preconcentrator for a protein sample with low concentration. The preconcentration chip was designed and fabricated using a polydimethylsiloxane replica through standard lithophotography. A glass substrate is silanized prior to functionalizing the nanoparticles for self-assembly at a designed region. Due to the overlap of electrical double layers in a nanofluidic channel, a concentration polarization effect can be achieved using an electric field. A nonlinear electrokinetic flow is induced, resulting in the fast accumulation of proteins in front of the induced ionic depletion zone, so called exclusion-enrichment effect. Thus, the protein sample can be driven by electroosmotic flow and accumulated at a specific location. The chip is used to collect fluorescein isothiocyanate-labeled bovine serum albumin (FITC-BSA) diluted in phosphate-buffered saline (PBS) buffer solution. Different concentrations of the buffer media were studied herein. Fluorescence intensity images show that the buffer concentration of 4 mM is more appropriate than all the other ones. The sample of FITC-BSA with an initial concentration of $10{\mu}M$ in the 4 mM PBS solution increases its concentration at the desired region by up to 50 times within 30 min, demonstrating the results in this investigation.

• 생명과학회지
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• 제30권2호
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• pp.113-121
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• 2020

대식세포는 특성에 따라 크게 classically activated macrophages (M1-phenotype macrophages)와 alternatively activated macrophages (M2-phenotype macrophages) 두 가지의 형태로 나눌 수 있다. M1 대식세포의 경우 직·간접적으로 병원체, 감염된 조직 및 암세포 등을 제거하는 능력을 가진 반면, M2 대식세포의 경우 항염증 반응을 동반한 손상된 세포 조직의 복구 및 세포외기질의 생성에 관여하고 있다. 본 연구에서는 상황버섯 열수추출물을 합성 흡착제인 Diaion HP-20에 통과시켜 소수성 물질을 제거한 시료(PLEP)을 이용하여 인간 유래 THP-1 단핵구 세포주의 염증성 혹은 항염증성 분극화 특성을 알아보았다. 먼저 PLEP 자체의 단핵구 세포에 대한 세포독성을 확인한 결과, 고농도의 300 ㎍/ml에서 세포독성이 확인되지 않았다. 한편 세포의 형태학적 변화를 확인한 결과, PLEP의 농도가 증가함에 따라 M1- phenotype 대식세포와 유사한 flatted and branched 형태가 증가하였다. 대식세포로 분화시킨 THP-1 세포주에 PLEP를 처리한 후, M1 대식세포 분극화 관련 유전자인 TNFα, IL-1β, IL-6, IL-8, CXCL10, CCR7과 M2-분극화 관련 유전자인 MRC-1, DC-SIGN, CCL17, CCL22의 유전자 발현량을 조사하여 분극화 양상을 알아보았다. 그 결과, M1-분극화 관련 유전자들은 PLEP 농도 의존적으로 증가하였지만, M2-분극화 관련 유전자들은 반대로 감소하였다. 또한 ELISA assay를 통하여 M1 분극화 관련 cytokine인 TNFα, IL-1β, IL-6의 발현량이 유전자의 발현량과 동일하게 증가하였다. 이러한 cytokine들의 분비를 촉진시키는 MAPK signaling 또한 PLEP의 농도가 증가함에 따라 촉진되었고 염증성 cytokine과 관련된 전사인자 NF-κB의 활성화도 증가하였다. 따라서 PLEP는 인간 유래 THP-1 세포주에서의 M1 대식세포 분극화를 통해 염증 반응을 유발하는 것으로 확인되어 염증을 촉진하는 천연물질로 이용할 수 있을 것으로 전망된다.

• Journal of Magnetics
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• 제15권2호
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• pp.51-55
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• 2010

The electronic and magnetic properties of Cu-doped GaN with a Cu concentration of 6.25% and 12.5% are examined theoretically using the full-potential linear muffin-tin orbital method. The magnetic moment of Cu atoms decreases with increasing Cu concentration. The spin-polarization of Cu atoms is reduced due to the Cu d-d interaction depending on the distance between the nearest neighbouring Cu atoms. Cu atoms exhibits a clustering tendency in GaN. For Cu-adsorbed GaN thin films with a surface coverage of 0.25, the ferromagnetic state is found to be the energetically favourable state with an induced magnetic moment of $0.54\;{\mu}_B$ per supercell.