• 한국진공학회:학술대회논문집
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• 한국진공학회 1998년도 제14회 학술발표회 논문개요집
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• pp.133-133
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• 1998

In the thin film alloy formation of the transition metals ion-beam-mixing technique forms a metastable structure which cannot be found in the arc-melted metal alloys. Sppecifically it is well known that the studies about the electronic structure of ion-beam-mixed alloys pprovide the useful information in understanding the metastable structures in the metal alloy. We studied the electronic change in the ion-beam-mixed ppt-Ct alloys by XppS and XANES. These analysis tools pprovide us information about the charge transfer in the valence band of intermetallic bonding. The multi-layered films were depposited on the SiO2 substrate by the sequential electron beam evapporation at a ppressure of less than 5$\times$10-7 Torr. These compprise of 4 ppairs of ppt and Cu layers where thicknesses of each layer were varied in order to change the alloy compposition. Ion-beam-mixing pprocess was carried out with 80 keV Ae+ ions with a dose of $1.5\times$ 1016 Ar+/cm2 at room tempperature. The core and valence level energy shift in these system were investigated by x-ray pphotoelectron sppectroscoppy(XppS) pphotoelectrons were excited by monochromatized Al K ａ(1486.6 eV) The ppass energy of the hemisppherical analyzer was 23.5 eV. Core-level binding energies were calibrated with the Fermi level edge. ppt L3-edge and Cu K-edge XANES sppectra were measured with the flourescence mode detector at the 3C1 beam line of the ppLS (ppohang light source). By using the change of White line(WL) area of the each metal sites and the core level shift we can obtain the information about the electrons pparticippating in the intermetallic bonding of the ion-beam-mixed alloys.

• 한국진공학회:학술대회논문집
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• 한국진공학회 2013년도 제44회 동계 정기학술대회 초록집
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• pp.658-658
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• 2013

Graphene is an attractive material for various device applications due to great electrical properties and chemical properties. However, lack of band gap is significant hurdle of graphene for future electrical device applications. In the past few years, several methods have been attempted to open and tune a band gap of graphene. For example, researchers try to fabricate graphene nanoribbon (GNR) using various templates or unzip the carbon nanotubes itself. However, these methods generate small driving currents or transconductances because of the large amount of scattering source at edge of GNRs. At 2009, Bai et al. introduced graphene nanomesh (GNM) structures which can open the band gap of large area graphene at room temperature with high current. However, this method is complex and only small area is possible. For practical applications, it needs more simple and large scale process. Herein, we introduce a photosensitive graphene device fabrication using CdSe QD coated nano-porous graphene (NPG). In our experiment, NPG was fabricated by thin film anodic aluminum oxide (AAO) film as an etching mask. First of all, we transfer the AAO on the graphene. And then, we etch the graphene using O2 reactive ion etching (RIE). Finally, we fabricate graphene device thorough photolithography process. We can control the length of NPG neckwidth from AAO pore widening time and RIE etching time. And we can increase size of NPG as large as 2 $cm^2$. Thin CdSe QD layer was deposited by spin coatingprocess. We carried out NPG structure by using field emission scanning electron microscopy (FE-SEM). And device measurements were done by Keithley 4200 SCS with 532 nm laser beam (5 mW) irradiation.

• Bulletin of the Korean Chemical Society
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• 제15권2호
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• pp.122-126
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• 1994

Corrosion of brass coated steel cords in the acetonitrile solution of sulfenamide derivatives, N-Cyclohexylbenzothiazole-2-sulfenamide (CBTS), N,N'-Dicyclohexylbenzothiazole-2-sulfenamide (DCBS), N-tert-Butylbenzothiazole-2-sulfenamide (TBBS), N-tert-Amylbenzothiazole-2-sulfenamide (TABS), and N-Oxydiethylbenzothiazole-2-sulfenamide (OBTS) was investigated by potentiostatic anodic and cathodic polarization (Tafel plot), DC polarization resistance, and AC impedance measurements. The corrosion current densities and rates are 1.236 ${\mu}A /cm^2$ and 0.655 MPY for CBTS; 1.881 ${\mu}A/cm^2$ and 0.988 MPY for DCBS; 2.367 ${\mu}A/cm^2$ and 1.257 MPY for TBBS; 3.398 ${\mu}A /cm^2$ and 1.809 MPY for TABS, respectively. OBTS among derivatives under study shows the lowest corrosion density (0.546 ${\mu}A /cm^2$) and the slowest corrosion rate (0.288 MPY). Also, the charge transfer resistances and the double layer capacitances are 275.21 $k{\Omega}{\cdot}cm^2$ and 7.0 ${\mu}F{cdot}cm^{-2}$ for CBTS; 14.24 ${\mu}F{\cdot}cm^2$ and 26 ${\mu}F{\cdot}cm^{-2}$ for DCBS; 54.15 $k{\Omega}{\cdot}cm^2$ and 26 ${\mu}F{\cdot}cm^{-2}$ for TBBS; 0.96$k{\Omega}{\cdot}cm^2$ and 83 ${\mu}F{\cdot}cm^{-2}$ for TABS, respectively. The weaker the electron donating inductive effect of derivatives is and the smaller the effect of steric hindrance is, the more the corrosion of brass coated steel cords in the acetonitrile solution of sulfenamide derivatives is prevented. The above results agree with that observed in the field of tire industry.

• Journal of Electrochemical Science and Technology
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• 제14권1호
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• pp.96-104
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• 2023

Synergistically increased oxygen evolution reaction (OER) of manganese oxide (MnO₂) catalyst is introduced with surface-modified halloysite nanotube (Fe₃O₄-HNTs) structure. The flake shaped MnO₂ catalyst is attached on the nanotube template (Fe₃O₄-HNTs) by series of wet chemical and hydrothermal method. The strong interaction between MnO₂ and Fe₃O₄-HNTs maximized active surface area and inter-connectivity for festinate charge transfer reaction for OER. The synergistical effect between Fe₃O₄ layer and MnO₂ catalyst enhance the Mn³⁺/Mn⁴⁺ ratio by partial replacement of Mn ions with Fe. The relatively increased Mn³⁺/Mn⁴⁺ ratio on MnO₂@FHNTs induced 𝜎^* orbital (e_g) occupation close to single electron, improving the OER performances. The MnO₂@FHNTs catalyst exhibited the reduced overpotential of 0.42 V (E vs. RHE) at 10 mA/cm² and Tafel slope of (99 mV/dec), compared with that of MnO₂ with unmodified HNTs (0.65 V, 219 mV/dec) and pristine MnO₂ (0.53 V, 205 mV/dec). The present study provides simple and innovative method to fabricate nano fiberized OER catalyst for a broad application of energy conversion and storage systems.

• 한국진공학회:학술대회논문집
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• 한국진공학회 2016년도 제50회 동계 정기학술대회 초록집
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• pp.286-286
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• 2016

Hexagonal boron nitride (hBN) is a dielectric insulator with a two-dimensional (2D) layered structure. It is an appealing substrate dielectric for many applications due to its favorable properties, such as a wide band gap energy, chemical inertness and high thermal conductivity[1]. Furthermore, its remarkable mechanical strength renders few-layered hBN a flexible and transparent substrate, ideal for next-generation electronics and optoelectronics in applications. However, the difficulty of preparing high quality large-area hBN films has hindered their widespread use. Generally, large-area hBN layers prepared by chemical vapor deposition (CVD) usually exhibit polycrystalline structures with a typical average grain size of several microns. It has been reported that grain boundaries or dislocations in hBN can degrade its electronic or mechanical properties. Accordingly, large-area single crystalline hBN layers are desired to fully realize the potential advantages of hBN in device applications. In this presentation, we report the growth and transfer of centimeter-sized, nearly single crystal hexagonal boron nitride (hBN) few-layer films using Ni(111) single crystal substrates. The hBN films were grown on Ni(111) substrates using atmospheric pressure chemical vapor deposition (APCVD). The grown films were transferred to arbitrary substrates via an electrochemical delamination technique, and remaining Ni(111) substrates were repeatedly re-used. The crystallinity of the grown films from the atomic to centimeter scale was confirmed based on transmission electron microscopy (TEM) and reflection high energy electron diffraction (RHEED). Careful study of the growth parameters was also carried out. Moreover, various characterizations confirmed that the grown films exhibited typical characteristics of hexagonal boron nitride layers over the entire area. Our results suggest that hBN can be widely used in various applications where large-area, high quality, and single crystalline 2D insulating layers are required.

• 마이크로전자및패키징학회지
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• 제23권4호
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• pp.87-92
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• 2016

전자소자의 방열모듈에서 두께 방향의 열방출 특성에 대한 중요성이 증가하고 있다. 금속과 금속의 본딩 및 유전체와 금속의 본딩 구조를 갖는 2가지 종류의 2층 층상재료를 제조한 후 두께 방향으로 열확산계수를 측정하였다. 금속(STS439)과 금속(Al6061)으로 이루어진 2층 층상재료에서는 섬광법(LFA)으로 열확산계수를 측정했을 때, 열흐름의 방향을 반대로 변화시켜도 열확산계수의 변화가 없었다. 그런데, 유전체(AlN-Polymer)와 금속(Al6061)의 2층 층상재료에서는 열흐름의 방향을 반대로 인가하였을 때 열확산계수는 17.5% 정도 다르게 나타났다. 유전체와 금속의 단면구조를 갖는 2층 층상재료에서, 금속에서 유전체 방향으로 측정한 열확산계수가 유전체에서 금속 방향으로 측정한 열확산계수에 비해 17.5% 작게 나타난 이유는, 금속내의 전자가 갖고 있던 에너지가 유전체 쪽으로 전달되기 위해서는 계면 주변에서 포논의 에너지 형태로 변환될 때 저항이 생기기 때문이다.

• 한국신재생에너지학회:학술대회논문집
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• 한국신재생에너지학회 2010년도 춘계학술대회 초록집
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• pp.87-87
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• 2010

Photoelectrochemical (PEC) systems are promising methods of producing H2 gas using solar energy in an aqueous solution. The photoelectrochemical properties of numerous metal oxides have been studied. Among them, the PEC systems based on TiO2 have been extensively studied. However, the drawback of a PEC system with TiO2 is that only ultraviolet (UV) light can be absorbed because of its large band gap (3.2 - 3.4 eV). Two approaches have been introduced in order to use PEC cells in the visible light region. The first method includes doping impurities, such as nitrogen, into TiO2, and this technique has been extensively studied in an attempt to narrow the band gap. In comparison, research on the second method, which includes visible light water splitting in molecular photosystems, has been slow. Mallouk et al. recently developed electrochemical water-splitting cells using the Ru(II) complex as the visible light photosensitizer. the dye-sensitized PEC cell consisted of a dye-sensitized TiO2 layer, a Pt counter electrode, and an aqueous solution between them. Under a visible light (< 3 eV) illumination, only the dye molecule absorbed the light and became excited because TiO2 had the wide band gap. The light absorption of the dye was followed by the transfer of an electron from the excited state (S*) of the dye to the conduction band (CB) of TiO2 and its subsequent transfer to the transparent conducting oxide (TCO). The electrons moved through the wire to the Pt, where the water reduction (or H2 evolution) occurred. The oxidized dye molecules caused the water oxidation because their HOMO level was below the H2O/O2 level. Organic dyes have been developed as metal-free alternatives to the Ru(II) complexes because of their tunable optical and electronic properties and low-cost manufacturing. Recently, organic dye molecules containing multi-branched, multi-anchoring groups have received a great deal of interest. In this work, tri-branched tri-anchoring organic dyes (Dye 2) were designed and applied to visible light water-splitting cells based on dye-sensitized TiO2 electrodes. Dye 2 had a molecular structure containing one donor (D) and three acceptor (A) groups, and each ended with an anchoring functionality. In comparison, mono-anchoring dyes (Dye 1) were also synthesized. The PEC response of the Dye 2-sensitized TiO2 film was much better than the Dye 1-sensitized or unsensitized TiO2 films.

• 대한화학회지
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• 제40권7호
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• pp.467-473
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• 1996

유기 전도성고분자들 중 100-400${\Omega}^{-1}cm^{-1}$으로 전도도가 큰 피롤 고분자는 공기 중에서 산화되어 전도성이 저하되는데, 이를 막기 위해 피롤을 먼저 일정량 중합한 후 산소에 내성이 큰 티오펜 고분자를 일정량 끼워심기 중합시켜 이와 같은 단점이 보완된 고분자 복합체를 만들고 그 때의 중합 속도를 측정하였다. 피롤 고분자를 먼저 1.70C$cm^{-2}$만큼 전기적으로 중합시킨 후 그 위에 티오펜 고분자를 0.34C$cm^{-2}$로 전기적 중합시켰을 때 그 산화-환원 특성이 개선되었으며, 3개월 동안 공기 중에 방치한 것의 순환 전압-전류 특성이 처음것과 잘 이치하였다. 티오펜의 중합 속도는 백금 전극 위에서 피롤 고분자를 1.70C$cm^{-2}$로 일정량을 입힌 전극에서 행했을 때 속도상수 값은 각각 $3.89{\times}10^{-8}$과 $6.07{\times}10^{-8}cms^{-1}$이었고, 표준속도상수는 각각 $5.16{\times}10^{-6}$ 과 $3.94{\times}10^{-4} cms^{-1}$이었다. 또, 피롤을 입힌 전극에서의 전극촉매속도는 $3.45{\times}10^{-3}cm^3mol^{-1}s^{-1}$이었다. 이와같이 피롤로 수식한 전극에서의 고정된 피롤 피막층은 촉매적 기능을 가지고 있음을 알 수 있고, 티오펜을 중합할 때의 반응은 고분자 피막 내에서 전하전달과 확산이 지배적인 과정이었다. 반면에 백금 전극에 티오펜을 중합할 때는 전자 전달이 지배적이 과정으로 나타났다.

• 폴리머
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• 제26권2호
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• pp.260-269
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• 2002

본 연구에서는 범용 열가소성수지인 폴리프로필렌에 다양한 입자 강화제로 무기질 폐기 제올라이트, 탈크, 탄산칼슘 등을 첨가하여 소재를 복합재료화 하였다. 또한 입자 사이즈에 따른 열안정성과 입자 강화제에 따른 난연 특성을 확인하였다. 본 연구에서는 입도 분석 결과 폐기 제올라이트가 85.34 $mu extrm{m}$, 탄산칼슘이 33.93 $mu extrm{m}$, 탈크가 18.51 $mu extrm{m}$의 평균 입자 크기를 가지고 있는 것을 확인하였다. 난연성 측정으로 산소지수(LOI, ASTM D2863)와 콘 칼로리미터 (ASTM E1354 ISO 5660)를 사용하였으며, 열 안정성 측정으로는 TGA를 사용하였다. 입자 강화제와 난연제 DBDPO를 사용한 결과 최대 열 방출 속도(M-HRR)는 탈크>탄산칼슘>폐기 제올라이트 순으로 감소됨을 확인하였다. 콘 칼로리미터 실험 결과, 난연제 DBDPO만 혼합하였을 경우보다 입자 강화제를 첨가 혼합하였을 경우가 난연 효율이 대략 2배 정도 향상됨을 확인하였다. 또한 산소지수 결과도 콘 칼로리미터와 유사한 경향을 보임을 확인하였다. 광학현미경(OM)과 주사전자현미경(SEM)을 사용하여 입자 강화된 복합재료의 연소되는 과정의 단면을 연소 단계별로 관찰함으로써 연소 표면에서의 입자 강화제의 배열 양상 및 산소 공급의 특성 등을 연구하였다.

• 생태와환경
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• 제57권2호
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• pp.61-74
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• 2024

낙동강 하구에 위치한 대마등은 모래톱으로 형성되어 있으며, 잘 발달된 조간대 갯벌을 갖고 있다. 본 연구에서는 2011년 1월부터 12월까지 대마등 갯벌에서 저서미세조류의 서식환경, 광합성 색소와 광합성률을 알아보았다. 퇴적물 공극수의 무기질소는 주로 암모늄염이고, 상부 수의 무기질소는 주로 질산염+아질산염으로 나타났다. Chlorophyll a 및 Fucoxanthin 농도는 퇴적물 표층이, 전체 퇴적층 평균값보다 현저히 높았다. 전체 조사기간 중 저서미세조류의 최대양자수율의 평균값은 0.52±0.03이었으며, 최고값은 2월(0.61±0.08)에 관측되었다. 최대전자전달률은 봄부터 초가을(4월에서 10월까지)까지는 높고 겨울에서 초봄(1월에서 3월 및 11월, 12월)까지는 낮은 계절적인 경향을 보였고, 최고값은 7월, 최저값은 1월에 나타났다. 시간별 저서미세조류의 최대 양자수율의 평균값은 0.48±0.03이었으며, 최고값(0.61±0.08)은 정오에 관측되었다. 최대전자전달률은 정오에 최고 값과 16시에 최저값을 보였다. 이로써 저서미세조류의 생산성은 조사시간 및 퇴적물 깊이에 따라 현저한 차이가 나타나므로 Diving-PAM을 사용하여 저서미세조류의 생산성을 정량화하기 위해서는 물때를 기준으로 조사가 이루어져야 하며, 동시에 퇴적물 층별 색소분석도 수행되어야 할 것으로 판단된다.