• 한국전기전자재료학회논문지
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• 제31권6호
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• pp.403-407
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• 2018

In this study, double layer KTN/STO thin films were fabricated on $Pt/Ti/SiO_2/Si$ substrate, their structural and electrical properties were measured according with the number of STO coatings, and their applicability to microwave materials was investigated. The average grain size was about 80~90 nm, the average thickness of the 6-coated KTN thin film was about 320 nm, and the average thickness of the STO thin film coated once was about 45~50 nm. The dielectric constant decreased with increasing frequency, and as the number of STO coatings increased, the rate of change of the dielectric constant with the applied electric field decreased. The tunability of the KTN thin film showed a maximum value of 19.8% at 3 V. The figure of merit of the KTN/1STO thin film was 9.8 at 3 V.

• Korean Chemical Engineering Research
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• 제43권1호
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• pp.92-97
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• 2005

본 연구에서는 음성 감광제를 이용하여 모형을 제작하고, PDMS(polydimethylsiloxane)로 본을 뜬 후에 유리와 접합시켜 마이크로채널을 제작하였다. 특히 PDMS의 접촉각 변화에 따른 마이크로채널에서 유체의 속도변화를 측정하기 위하여, PDMS의 표면을 플라즈마를 이용하여 처리하였다. 표면처리된 PDMS의 접촉각은 $19^{\circ}$, $46^{\circ}$ 그리고 $69^{\circ}$였으며, 미처리된 PDMS의 접촉각은 $105^{\circ}$였다. 표면처리된 PDMS와 플라즈마 처리를 하지 않은 PDMS에 대하여 외부전압을 변화시켜서 마이크로채널에서의 유체의 속도를 측정하였다. 그 결과 동일한 접촉각을 갖는 PDMS에 대하여 외부전압을 변경시켰을 때, 외부전압이 증가할수록 유체의 속도가 비선형적으로 증가하였다. 이는 외부전압이 증가할수록 계면에서의 전하밀도가 증가하게 되고, 이로 인하여 전기이중층이 압축되어 표면전위가 증가하며, 따라서 제타전위의 값이 증가하기 때문인 것으로 해석된다. 또한, 동일한 외부전압에서 PDMS의 접촉각이 가장 작은 $19^{\circ}$일 때 유체의 속도가 가장 빠르게 나타났다. 이는 유체와 PDMS의 부착 정도에 따라 전기이중층 두께가 달라지고, 이러한 두께변화가 결과적으로 동일한 외부전압에서 접촉각의 크기에 따라 유체의 속도차이를 가져오는 것으로 사료된다.

• 마이크로전자및패키징학회지
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• 제15권2호
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• pp.23-28
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• 2008

최적 소자구조에 의한 고분자 발광다이오드의 외부 양자효율 향상을 위해 스핀코팅 방법으로 ITO/EDOT:PSS/(PFO)/PFO:MEH-PPV/LiF/Al 구조의 발광소자를 제작하고 전기, 광학적 특성을 조사하였다. ITO(indium tin oxide) 투명전극을 양극으로 사용하고 정공수송층으로 PEDOT:PSS[poly(3,4-ethylenedioxythiophene):poly(styrene sulfolnate)]를 사용하였으며, 발광물질로는 PFO[poly(9,9-dioctyl-fluorene)]와 MEH-PPV [poly(2-methoxy-5(2-ethylhexoxy)-1,4-phenylenevinyle)]를 각각 호스트와 도펀트로 사용하였다. PFO:MEH-PPV 발광층의 두께를 약 $400{\AA}$으로 형성하였고, MEH-PPV의 농도는 9wt%로 고정하여 도핑하였다. PFO 발광층의 두께를 $200{\sim}300{\AA}$의 범위로 변화시켜 전계발광 특성을 비교 해 본 결과, 두께가 약 $250{\AA}$ 부근에서 가장 우수한 광학적 특성이 관찰되었으며, 13V의 인가전압에서 각각 약 $400mA/cm^2$의 전류밀도와 $1500cd/m^2$의 휘도가 관찰되었다 또한 PFO 발광층을 2중으로 구성한 소자(PFO/PFO:MEH-PPV)가 단일 발광층을 갖는 소자 (PFO:MEH-PPV)에 비해 발광휘도 및 전류 효율에서 약 3배의 향상된 특성을 보여주었다.

• 한국표면공학회지
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• 제29권6호
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• pp.847-850
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• 1996

The bi-layered films composed of Co-Cr-Ta layers and paramagnetic $Co_{67}Cr_{33}$ underlayer were deposited by suing Facing Targets Sputtering(FTS). The effects of $Co_{67}Cr_{33}$ underlayer on the crystallographic and magnetic characteristics of the Co-Cr-Ta layer deposited on the underlayer was investigated. The diffraction intensity $I_{p(002)}$ of Co-Cr-Ta layers on the $Co_{67}Cr_{33}$ layer was stronger than that of single layer and Co-Cr-Ta/Ti double layer. Therefore, the crystallinity of Co-Cr-Ta layer was imporved by the $Co_{67}Cr_{33}$ underlayer rather than Ti ones. However, te coercivity H$_{c\bot}$ of Co-Cr-Ta layers deposited on $Co_{67}Cr_{33}$ underlayer was as low as 250 Oe even at substrate temperature of $220^{\circ}C$. This H$_{c\bot}$ decrease seems to be attributed to the effect of the $Co_{67}Cr_{33}$ underlayer as well as interval time between deposition of the underlayer and the Co-Cr-Ta layer.

• 한국전자파학회논문지
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• 제21권2호
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• pp.194-201
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• 2010

본 논문에서는 CDMA/RFID 주파수 격리도 향상을 위해 double split ring resonator(DSRR)을 이용한 주파수 선택적 표면(FSS)을 설계하였다. 제안된 FSS의 단위 셀 구조는 외부 SRR과 내부 SRR로 구성되며, 이 두 SRR의 gap은 같은 방향에 위치한다. SRR의 gap 간격 및 line 두께 등을 조절하여 전체적인 크기를 유지하면서 공진 주파수 및 스커트 특성을 조절할 수 있다. 동작 주파수에서 제안된 SRR의 필드는 magneto-dielectric SRR과 다른 방향을 가진다. 한 층은 $9{\times}9$ 단위 셀로 구성되어 있으며, 50 mm 간격을 두고 다른 층이 위치해 있다. 시뮬레이션 결과를 검증하기 위해 패치 안테나 및 FSS를 제작했으며, 측정 결과는 시뮬레이션 결과와 유사한 경향을 보인다. 단위 셀의 저지 대역에서의 전기적 크기는 $0.110\;{\lambda}{\times}0.110\;{\lambda}{\times}0.002\;{\lambda}$로 다이폴 FSS에 비해 소형이며, 지지대를 포함한 2층 FSS의 크기는 $1.058\;{\lambda}{\times}1.058\;{\lambda}{\times}0.153\;{\lambda}$이다. 측정 결과 CDMA 대역의 이득이 유지되며, RFID 대역에서 6.9 dB 이득이 감소하였다.

• 한국전기전자재료학회논문지
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• 제27권9호
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• pp.571-575
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• 2014

We synthesized new materials of $Zn(HPB)_2$ and Ir-complexes as blue or red emitting material. We fabricated white Organic Light Emitting Diodes (OLED) by using $Zn(HPB)_2$ for the blue emitting layer, Ir-complexes for the red emitting layer and $Alq_3$ for the green emitting layer. We fabricated white OLED by using double emitting layers of $Zn(HPB)_2$:Ir-complexes and $Alq_3$. The doping rate of Ir-complexes was varied, such as 0.2%, 0.4%, 0.6%, and 0.8%, respectively. When the doping rate of $Zn(HPB)_2$:Ir-complexes was 0.6%, white emission was achieved. The Commission Internationale de l'Eclairage (CIE) coordinates of the white emission was (0.322, 0.312).

• 한국전기전자재료학회논문지
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• 제20권10호
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• pp.873-877
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• 2007

In order to apply a complex multilayer chip LC filter, this study has estimated the interfacial reaction and coupling properties of dielectric materials $Pb(Fe_{1/2}Nb_{1/2})O_3$ and Ni-Zn-Cu ferrite materials through low-temperature co-sintering (LTCS). PFN powders were fabricated using double calcinated at $700^{\circ}C$ and then $850^{\circ}C$. While the perovskite phase rate was found to be 91 %, after heat treatment at $900^{\circ}C$ for 6h, the perovskite phase rate and density exhibited a value of 100 % and 7.46$g/cm^3$, respectively. The PFN/Ni-Zn-Cu ferrite, PFN/CUO (or $Pb_2Fe_2O_5$) and ferrite/CuO (or $Pb_2Fe_2O_5$) were mechanically coupled through interfacial reactions after the specimen was co-sintered at $900^{\circ}C$ for 6 h. No intermediate layer exists for the mutual coupling reaction. This result indicates the possibility of low-temperature co-sintering without any interfacial reaction layer for a multilayer chip LC filter.

• 한국전기전자재료학회:학술대회논문집
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• 한국전기전자재료학회 1999년도 춘계학술대회 논문집
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• pp.193-196
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• 1999

Organic electroluminescent devices have attracted a great deal of attention due to thier potential application to full-color flat-panel displays. The 8-hydroxyquinollne Zinc(Znq$_2$) were synthesized successfully from zinc chloride(ZnCl$_2$) and zinc acetate(Zn(C$_2$H$_3$O$_3$)$_2$) as green omitting material. A double-layer ELD consist of an emitting layer of B-hydroxyquinoline Zinc(Znq$_2$) and a hole-transport layer of tai-phenylene diamine(TPD) derivatives sandwiched between an Aluminium(Al) and Indium-Tin-Oxide(ITO) electrodes omitted green light resulting from Znq$_2$. The electroluminescent devices (ELD) exhibited a maximum luminance of 1000cd/$\textrm{cm}^2$ at a driving voltage of 8V and a driving current density of 0.4mA/$\textrm{cm}^2$.

• Journal of Communications and Networks
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• 제14권5호
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• pp.566-577
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• 2012

In randomly deployed networks, such as sensor networks, an important problem for each node is to discover its neighbor nodes so that the connectivity amongst nodes can be established. In this paper, we consider this problem by incorporating the physical layer parameters in contrast to the most of the previous work which assumed a collision channel. Specifically, the pilot signals that nodes transmit are successfully decoded if the strength of the received signal relative to the interference is sufficiently high. Thus, each node must extract signal parameter information from the superposition of an unknown number of received signals. This problem falls naturally in the purview of random set theory (RST) which generalizes standard probability theory by assigning sets, rather than values, to random outcomes. The contributions in the paper are twofold: First, we introduce the realistic effect of physical layer considerations in the evaluation of the performance of logical discovery algorithms; such an introduction is necessary for the accurate assessment of how an algorithm performs. Secondly, given the double uncertainty of the environment (that is, the lack of knowledge of the number of neighbors along with the lack of knowledge of the individual signal parameters), we adopt the viewpoint of RST and demonstrate its advantage relative to classical matched filter detection method.

• 한국전기전자재료학회논문지
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• 제20권6호
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• pp.502-507
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• 2007

The oxidation treatment of several carbon materials with a sodium chlorate and 70 wt.% of nitric acid, combined with heat treatment, were attempted to achieve an electrochemical active material with a larger capacitance. Among pitch, needle coke, calcinated needle coke and natural graphite, the structure of needle coke and calacinated needle coke were changed to the graphite oxide structure with the expansion of the inter-layer. On the other hand, the calcinated needle coke after oxidation and heating at $200^{\circ}C$ has exhibited largest capacitance per weight and volume of 29.5 F/g and 24.5 F/ml at the two-electrode system in the potential range of 0 to 2.5 V. The electrochemical performance of the calcinated needle coke was discussed with the phenomenon of the electric field activation and the formation of new pores between the expanded inter-layer at first charge.