• Journal of the Korean Institute of Electrical and Electronic Material Engineers
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• v.17 no.3
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• pp.278-282
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• 2004

The Hydrogenated amorphous carbon(a-C:H) thin films are deposited on silicon with a close field unbalanced magnetron(CFUBM) sputtering systems. The experimental data are obtained on the depositon rate and physical properties of a-C:H films using DC bias voltage and Ar/C$_2$H$_2$ pressure. The depostion rate and the surface roughness decrease with DC bias voltage, but the hardness of the thin films increases with DC bias voltage. And the position of G-peak moves to lower wavenumber indicating an increase in diamond-like carbon characteristics with the lower Ar/C$_2$H$_2$ pressure.

• Journal of Magnetics
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• v.15 no.3
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• pp.132-137
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• 2010

Plasma etching of $SiO_2$ contact holes was statistically analyzed by a fractional factorial experimental design. The analysis revealed the dependence of the etch rate and DC self-bias voltage on the input factors of the magnetically enhanced reactive ion etching reactor, including gas pressure, magnetic field, and the gas flow rates of $CHF_3$, $CF_4$, and Ar. Empirical models of the DC self-bias voltage and etch rate were obtained. The DC self-bias voltage was found to be determined mainly by the operating pressure and the magnetic field, and the etch rate was related mainly to the pressure and the flow rates of Ar and $CHF_3$.

• 한국정보디스플레이학회:학술대회논문집
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• 2005.07a
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• pp.513-514
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• 2005

In plasma processing reactors, it is common practice to control plasma density and ion bombardment energy by manipulating excitation voltage and frequency. In this paper, a dually excited capacitively coupled rf plasma reactor is self-consistently simulated with a three moment model. Effects of phase differences between primary and secondary voltage waves, simultaneously modulated at various combination of commensurate frequencies, on plasma properties are investigated. The simulation results show that plasma potential and density as well as primary self-dc bias are nearly unaffected by the phase lag between the primary and the secondary voltage waves. The results also show that, with the secondary frequency substantially lower than the primary frequency, secondary self-dc bias remains constant regardless of the phase lag. As the secondary frequency approaches to the primary frequency, however, the secondary self-dc bias becomes greatly altered by the phase lag, and so does the ion bombardment energy at the secondary electrode. These results demonstrate that ion bombardment energy can be more carefully controlled through plasma simulation.

• Proceedings of the Korea Institute of Applied Superconductivity and Cryogenics Conference
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• 2003.10a
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• pp.113-116
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• 2003

Confluence buffers and single flux quantum (SFQ) switches are essential components in constructing a high speed superconductive Arithmetic Logic Unit (ALU). In this work, we developed a SFQ confluence buffer and an SFQ switch. It is very important to optimize the circuit parameters of a confluence buffer and an SFQ switch to implement them into an ALU. The confluence buffer that we are currently using has a small bias margin of $\pm$11％. By optimizing it with a Josephson circuit simulator, we improved the design of confluence buffer. Our simulation study showed that we improved bias global margin of 10％ more than the existent confluence buffer. In simulations, the minimal bias margin was $\pm$33％. We also designed, fabricated, and tested an SFQ switch operating in a DC mode. The mask layout used to fabricate the SFQ switch was obtained after circuit optimization. The test results of our SFQ switch showed that it operated correctly and had a reasonably wide margin of $\pm$15％.

• Journal of the Semiconductor & Display Technology
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• v.4 no.2 s.11
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• pp.11-14
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• 2005

In plasma processing reactors, it is common practice to control plasma density and ion bombardment energy by manipulating excitation voltage and frequency. In this paper, a dually excited capacitively coupled rf plasma reactor is self-consistently simulated with a three moment model. Effects of phase differences between primary and secondary voltage waves, simultaneously modulated at various combinations of commensurate frequencies, on plasma properties are investigated. The simulation results show that plasma potential and density as well as primary self-dc bias are nearly unaffected by the phase lag between the primary and the secondary voltage waves. The results also show that, with the secondary frequency substantially lower than the primary frequency, secondary self·do bias remains constant regardless of the phase lag. As the secondary frequency approaches to the primary frequency, however, the secondary self-dc bias becomes greatly altered by the phase lag, and so does the ion bombardment energy at the secondary electrode. These results demonstrate that ion bombardment energy can be more carefully controlled through plasma simulation.

• Journal of Communications and Networks
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• v.14 no.5
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• pp.540-545
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• 2012

In this paper, the lagged cross-correlation of two probability density functions constructed by kernel density estimation is proposed, and by maximizing the proposed function, adaptive filtering algorithms for supervised and unsupervised training are also introduced. From the results of simulation for blind equalization applications in multipath channels with impulsive and slowly varying direct current (DC) bias noise, it is observed that Gaussian kernel of the proposed algorithm cuts out the large errors due to impulsive noise, and the output affected by the DC bias noise can be effectively controlled by the lag ${\tau}$ intrinsically embedded in the proposed function.

• The Journal of Korean Institute of Communications and Information Sciences
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• v.37A no.12
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• pp.1038-1042
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• 2012

In this paper, a new distance measure for biased PDFs is proposed and a related equalizer algorithm is also derived for supervised adaptive equalization for multipath channels with impulsive and time-varying DC bias noise. From the simulation results in the non-Gaussian noise environments, the proposed algorithm has proven not only robust to impulsive noise but also to have the capability of cancelling time-varying DC bias noise effectively.

• Proceedings of the Korean Vacuum Society Conference
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• 2013.08a
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• pp.253.1-253.1
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• 2013

RF 마그네트론 스퍼터링법으로 증착된 Al-doped ZnO 박막을 씨드층으로 하고, zinc nitrate hexahydrate, hexamethylenetetramine (HMTA), ammonium chloride (AC) 및 polyethyleneimine (PEI)를 반응용액으로 한 수열합성법으로 ZnO 나노와이어를 성장시켰다. ZnO 나노와이어의 성장 공정 중 반응 용액내에 DC 바이어스를 인가하고, DC 바이어스의 인가 유무 및 인가 DC 바이어스 전압의 크기 변화에 따라 성장시킨 ZnO 나노와이어의 특성을 비교분석하였다. 다양한 공정변수 변화에 따라 수열합성법으로 성장시킨 ZnO 나노와이어 시편들을 SEM 분석을 통해 특성분석을 수행하였다.

• Journal of the Microelectronics and Packaging Society
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• v.12 no.3 s.36
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• pp.207-212
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• 2005

Al, Ti, Ta, and Cr thin films were deposited on a polyimide substrate using DC magnetron sputter to study the adhesion characteristics of metal films on polyimide substrates, while RF bias of 0 - 400 W was applied to the substrate during DC sputtering. The adhesion strength was evaluated using a 90-degree peel test. The peel tests showed that the adhesion strength was enhanced by applying the RF bias to the substrate in all specimens. Scanning electron microscopy and Auger depth profile of the fractured surfaces indicate that the polyimide underwent cohesive failure during peeling and heavy deformation was also observed in the metal films peeled from the polyimide substrate when the RF bias applied during the deposition. Cross-sectional transmission electron microscopy revealed that the metal/polyimide interface was not clear and complicated. This complicated interface, likely formed due to the RF bias applied to the substrate, was attributed to the adhesion enhancement observed during the bias sputtering.

• Proceedings of the Korean Institute of Surface Engineering Conference
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• 2016.11a
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• pp.102-102
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• 2016

본 연구에서는 직류 전원(direct current; DC)을 이용한 스퍼터링과 고전력펄스 마그네트론 스퍼터링(high-power impulse magentron sputtering; HIPIMS)의 두 가지 방법과 빗각 증착을 적용하여 제조한 티타늄 질화물(TiN) 박막의 미세구조 변화가 물성에 미치는 영향을 확인하였다. TiN 박막은 99.5%의 Ti 타겟을 사용하고, Ar가스와 $N_2$ 분위기에서 스테인리스(SUS304)와 초경(cdmented carbide; WC-10wt.%Co) 기판위에 코팅하였다. 기판은 알코올과 아세톤으로 초음파 세척을 실시한 후 진공용기에 장착하고 기본 진공도인 ${\sim}2.0{\times}10^{-5}Torr$ 까지 진공배기를 실시하였다. 기판과 타겟 간의 거리는 DC 스퍼터링은 10 cm, HIPIMS 스퍼터링은 8.5 cm 이었다. 진공용기의 압력이 기본 진공도까지 배기되면 Ar 가스를 ${\sim}10^{-2}Torr$로 주입한 후 기판에 라디오 주파수(radio frequency; RF) 전원으로 약 -800 V의 전압을 인가하여 글로우 방전을 발생시키고 약 30 분간 청정을 실시하였다. 기판의 청정이 끝난 후 기본 진공도까지 배기한 후 Ar와 $N_2$ 가스를 ${\sim}10^{-3}Torr$로 주입하여 TiN 코팅을 실시하였다. 빗각의 크기는 $45^{\circ}$와 $-45^{\circ}$이며, TiN 박막의 총 두께는 약 $2.5{\sim}4.0{\mu}m$ 로 유지하였다. 공정조건에 따라 TiN 박막의 주상정은 형태와 기울어진 각도가 다른 것을 확인하였다. DC 스퍼터링으로 제조된 TiN 박막은 기판홀더에 약 -100 V 의 bias 전압을 인가하면 인가하지 않은 박막에 비해 치밀한 박막의 성장과 경도 값도 증가하는 사실을 확인하였다. 또한 빗각을 적용하고 bias 전압을 인가하지 않은 시편에서 박리현상이 일어났다. HIPIMS로 제조한 TiN 박막은 bias 전압을 인가한 박막과 인가하지 않은 박막의 주상정 형상과 경도 값에 큰 차이가 없었으며, 박막의 박리현상은 모든 시편에서 일어나지 않았다. DC 스퍼터링으로 제조한 TiN 박막은 bias 전압을 인가하지 않으면 색상이 노란색이 아닌 갈색으로 나타났으며, HIPIMS으로 제조한 박막은 bias 전압 인가 유무에 상관없이 노란색 색상을 나타냈다. 앞서 설명한 DC 스퍼터링과 HIPIMS의 공정조건에 따라 나타난 박막의 경도, 색상, 물성변화 차이는 DC 스퍼터링보다 높은 HIPIMS의 이온화율에서 기인한 것으로 생각된다. 본 연구결과를 이용하면 다양한 형태의 박막 구조 제어가 가능하고 이러한 미세구조 제어를 통해서 박막의 물성도 제어가 가능할 것으로 판단된다.