• Proceedings of the Korean Institute of Surface Engineering Conference
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• 2017.05a
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• pp.107-107
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• 2017

전자제품의 성능이 향상됨에 따라서 전자제품에 사용되는 부품의 고집적화가 필연적으로 요구되고 있으며, 고집적화 된 전자제품의 방열(heat dissipation)에 관한 문제점이 대두되고 있다. 방열은 전자기기의 성능과 수명을 유지하는데 있어서 중요한 문제 중 하나로서 방열 효과를 높이기 위해 다양한 연구 개발이 진행 중이다. 방열에 사용되는 소재로는 Cu가 있으며, 저렴한 가격과 상대적으로 높은 방열 효율을 가지는 장점이 있다. Cu는 전기 도금 증착 방법을 사용하여왔으나, 전기도금 방식으로 증착된 Cu 방열판은 제품에 열이 축적될 경우 Cu와 substrate 사이의 residual stress로 인해 박리나 뒤틀림 현상 등이 발생하여 high power를 사용하는 device의 방열 소재로 사용하기에는 개선해야 할 문제점이 있다. 이러한 문제점을 극복하기 위한 방법으로 magnetron sputter 증착 방법이 있으며, magnetron sputter은 대면적화가 용이하고, 다양한 물질의 증착이 가능한 장점으로 인해 hard coating 또는 thin film 증착과 같은 공정에 사용되고 있다. 특히 증착된 film의 특성을 조절하기 위해서 magnetron sputter에 pulse 또는 ICP (inductively coupled plasma) assisted 등을 적용하여 plasma 특성을 조절하는 방법 등에 관한 연구가 보고되고 있다. 본 연구에서는 pulsed magnetron sputtering 방식을 이용하여 증착된 Cu film 특성 변화를 확인하였다. 다양한 pulsing frequency와 pulsing duty ratio 조건에서, Si substrate 위에 증착된 Cu film과의 residual stress 변화를 측정하였다. Pulse duty ratio가 90% 에서 60%로 감소함에 따라서 Cu film의 residual stress가 감소하였고, pulsing frequency가 증가함에 따라 Cu film의 residual stress가 감소하는 것을 확인하였다. 증착 조건에 따른 plasma의 특성 분석을 위하여 oscilloscope를 이용하여 voltage와 current를 측정하였고, Plasma Sampling Mass spectrometer 를 이용하여 ion energy의 변화를 측정하였다. 이를 통해 plasma 특성 변화가 증착된 Cu film에 미치는 영향과 residual stress의 변화에 대한 연관성에 대하여 확인할 수 있었다.

• Applied Science and Convergence Technology
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• v.23 no.3
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• pp.145-150
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• 2014

MgO thin films were deposited by internal ICP-assisted reactive-magnetron sputtering with bipolar pulse bias on a substrate to suppress random arcs. Mg is reactively sputtered by a bipolar pulsed DC power of 100 kHz into ICP generated by a dielectrically shielded internal antenna. At a mass flow ratio of $Ar/O_2$ = 10 : 2 and an ICP/sputter power ratio of 1 : 1, optimal film properties were obtained (a powder-like crystal orientation distribution and a RMS surface roughness of approximately 0.42 nm). A bipolar pulse substrate bias at a proper frequency (~a few kHz) prevented random arc events. The crystalline preferred orientations varied between the (111), (200) and (220) orientations. By optimizing the plasma conditions, films having similar bulk crystallinity characteristics (JCPDS data) were successfully obtained.

• Proceedings of the Korean Vacuum Society Conference
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• 2010.02a
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• pp.193-193
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• 2010

HIPIMS(High sputtering impulse magnetron sputtering)은 수십 ${\mu}s$의 짧은 pulse 동안 수kw의 매우 높은 파워를 인가할 수 있어 밀도 $10^{13}/cm^3$ 이상의 고밀도 플라즈마 방전이 가능하여 스퍼터된 타겟 이온들의 이온화율이 매우 높은 특징을 가진다. HIPIMS를 통해 증착한 박막의 경우 매우 치밀한 조직을 가지고 있어 기존 DC, Pulsed DC, RF 증착을 통한 박막에 비해 우수한 물성을 보여준다. 본 실험에서는 대면적의 고품위 Al:ZnO 박막을 증착하기위하여 HIPIMS 증착법을 사용하였다. 1000mm폭 타겟상에서 균일한 증착을 위하여 Balanced B-field, Unbalanced field를 각각 인가하여 실험하였다. 시뮬레이션을 통하여 타겟 중심부와 가장자리의 자기장을 결정하였으며, target edge에서의 증착율과 cathode erosion 방지를 위하여 원형 트랙형으로 보조 자석을 설치하였다. $Al_2O_3$(2wt%)가 첨가된 planar target을 사용하였고, power는 700 W~2 kW, 그리고 pulse 폭은 $50-150 {\mu}s$정도로 변화시켜 가면서 상온에서 증착하였다. 플라즈마 가스로는 Ar만을 사용하여 두께는 60-100 nm정도로 증착하였다. Plasma emission monitoring을 통해 측정한 결과 Balanced B-field 에 비해 Unbalanced B-field 조건 에서 스퍼터된 이온들의 균일도가 우수하였으며 증착된 박막의 균일도 또한 증가하였다.

• Journal of Surface Science and Engineering
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• v.45 no.5
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• pp.206-211
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• 2012

Process analysis was carried out during deposition of MgO by inductively coupled plasma assisted reactive magnetron sputtering in Ar and $O_2$ ambient. At the initiation of Mg sputtering with bipolar pulsed dc power in Ar ambient, total pressure showed sharp increase and then slow fall. To analyse partial pressure change, QMS was used in downstream region, where the total pressure was maintained as low as $10^{-5}$ Torr during plasma processing, good for ion source and quadrupole operation. At base pressure, the major impurity was $H_2O$ and the second major impurity was $CO/N_2$ about 10%. During sputtering of Mg in Ar, $H_2$ soared up to 10.7% of Ar and remained as the major impurity during all the later process time. When $O_2$ was mixed with Ar, the partial pressure of Ar decreased in proportion to $O_2$ flow rate and that of $H_2$ dropped down to 2%. It was understood as Mg target surface was oxidized to stop $H_2$ emission by Ar ion sputtering. With ICP turned on, the major impurity $H_2$ was converted into $H_2O$ consuming $O_2$ and C was also oxidized to evolve CO and $CO_2$.

• Journal of the Korean Ceramic Society
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• v.43 no.2 s.285
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• pp.79-84
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• 2006

We studied the microstructure and magnetic property of the pulsed DC magnetron sputtered $Zn_{\0.8}Co_{0.2}O$ film as a function of substrate temperatures. The X-ray patterns of the $Zn_{\0.8}Co_{0.2}O$ film showed a strong (002) preferential orientation at $500^{\circ}C$. The films with a crystallite size of 23-35 nm were grown in the form of nano-sized structure and this tendency was remarkable with increasing substrate temperature. The UV-visible result showed that the $Zn_{\0.8}Co_{0.2}O$ film prepared above $300^{\circ}C$ has a high optical transmittance of over $80\%$ in the visible region. The absorption bands were observed due to sp-d interchange action by $Co^{2+}$ complex ion and dd transition in the region from 500 to 700nm. The resistivity of the film was below $10^{-1}\;\Omega-cm\;above\;300^{\circ}C$. The AGM analysis results for the all films showed the magnetic hysteresis curves of ferromagnetic nature. The low electrical resistivity and room temperature ferromagnetism of ZnCoO thin films 'deposited above $300^{\circ}C$ suggested the possibility for the application to Diluted Magnetic Semiconductors (DMSs).

• Proceedings of the Korean Institute of Surface Engineering Conference
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• 2008.11a
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• pp.23-24
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• 2008

Bipolar pulsed dc magnetron sputtering을 이용하여 태양전지의 투명 전도막용으로 유리기판 위에 Al doped ZnO (AZO) 박막을 증착하였다. $400{\times}400\;mm$의 대면적 기판에 증착하기 위해서 $5{\times}25$ inch 대형 사각 AZO target (Al 2 wt%)을 사용했고, $50{\sim}250\;kHz$의 bipolar pulse를 인가하였다. 실제로는 $400{\times}400\;mm$ 면적의 기판에 slide glass 16개를 사용했으며, 약 700 nm 두께에서 두께와 투과도, 비저항의 균일도를 평가하였다. Bipolar pulse의 주파수 150 kHz일 때, 가장 우수한 특성을 갖는 AZO가 증착되었으며, $2.13{\times}10^{-3}{\Omega}{\cdot}cm$의 비저항에 가시광선 영역에서 82%의 투과율을 보였다. 또한, $400{\times}400\;mm$ 대면적 기판에서의 두께와 투과도, 비저항의 불균일도는 각각 5%, 1%, 9% 였다.

• Progress in Superconductivity and Cryogenics
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• v.6 no.4
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• pp.1-4
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• 2004

Three group samples with difference thickness of $CeO_2$ capping layer deposited by PLD were studied. Among them, one group $CeO_2$ films were deposited on stainless steel tape coated with IBAD- YSZ and $CeO_2$ buffer layer ($CeO_2$/IBAD-YSZ/SS); other two groups of $CeO_2 YSZ Y_2O_3$multi-layer were deposited on NiW substrates for fabrication of YBCO coated conductor through RABiTS approach. The pulsed laser deposition (PLD) and DC magnetron sputtering were employed to deposit these buffer layers. On the top of buffer layer, YBCO film was deposited by PLD. The effect of thickness of $CeO_2$ film on the texture of $CeO_2$ film and critical current density ($J_c$) of YBCO film were analyzed. For the case $CeO_2$ on $CeO_2$/IBAD-YSZ/SS, there was a self-epitaxy effect with the increase of $CeO_2$ film. For $YSZ/Y_2O_3$ NiW which was deposited by PLD or DC magnetron sputtering, there is not self-epitaxy effect. However, the capping layer of $CeO_2$ film deposited by PLD improved the quality of buffer layer for $YSZ/Y_2O_3$ which was deposited by DC magnetron sputtering, therefore increased the $J_c$ of YBCO film.

• Journal of Surface Science and Engineering
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• v.40 no.5
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• pp.209-213
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• 2007

Change of the plasma volume by pulse frequency in a bipolar pulsed DC unbalanced magnetron sputtering was investigated. As increasing the frequency at off duty 10% and at a constant power, the plasma volume was lengthened in vertical direction from the AZO target. When there is an electrically floated substrate, the vertical length of the plasma area was not affected by the pulse frequency. Instead, the diameter of the plasma volume was increased. We found that the temperature rise of a substrate was affected by the pulse frequency, too. As increasing it, the maximum temperature rise of a glass substrate was decreased from $132^{\circ}C\;to\;108^{\circ}C$.

• Proceedings of the Korean Vacuum Society Conference
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• 2009.02a
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• pp.255.1-255.1
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• 2009

• Proceedings of the Korean Magnestics Society Conference
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• 2004.06a
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• pp.82-83
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• 2004