• Journal of the Korean institute of surface engineering
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• v.41 no.3
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• pp.94-101
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• 2008

A new convenient magnet array module is designed to investigate effects of magnetic field array on magnetron discharge characteristics. Magnetic field analysis showed good agreement of measured discharge region by a CCD device which has a high quantum efficiency over visible wavelength range. OES (optical emission spectroscopy) showed major emission peaks are from electronic transitions in 400 nm range and 800 nm range. Effects of driving voltage characteristics were analyzed in a point of electron drift trajectories and ionizing collision frequencies. Pulsed dc with a fast rising and falling time was analyzed to have potential to increase ionization collisions by putting a burst of hot electrons and to raise sheath potential. From measured voltage and current waveform, maximum of -1000 V peak was generated with $-400\;V_{rms}$ conditions. Possibility of a properly designed magnetron cathode was shown to be used as a melting device. Cu was successfully melted with power density of a several tens of $W/cm^2$.

• 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.

• Journal of the Korean Ceramic Society
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• v.51 no.5
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• pp.447-452
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• 2014

This paper presents the effects of pulse plasma parameters such as duty cycle and pulse frequency on the properties of TiAlN coatings deposited by asymmetric bipolar pulsed DC magnetron sputtering systems. The results show that, with decreasing duty cycle and increasing pulse frequency, the coating morphology changes from a columnar structure to a dense structure with finer grains. Pulsed sputtered TiAlN coatings showed higher hardness, higher residual stress, and smaller grain sizes than did DC prepared TiAlN coatings. Moreover, residual stress and nanoindentation hardness of pulsed sputtered TiAlN coatings increased with increasing pulse frequency. Meanwhile, the surface roughness decreased continuously with increasing pulsed DC frequency up to 50 kHz.

• 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.

• Proceedings of the KIEE Conference
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• 2003.07c
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• pp.1732-1734
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• 2003

An MgO thin film sputtering system for the PDP (Plasma Display Panel) applications has been developed. This system was manufactured with a vertical In-Line type of 42 inch, which has the length of 520 mm and the width of 900 mm. A reactive magnetron discharge for this sputtering was generated using an unipolar pulsed power supply which has functions of constant voltage (Max. 500 V) and current (Max. 15 A) control, frequency of $10{\sim}100$ kHz and duty ratio of $10{\sim}60$ %. The experiment was conducted under various conditions : $3{\sim}10$ mTorr of pressure, the ratio of $O_2$/Ar = $0.1{\sim}0.5$, 50 % of duty and power of $0.5{\sim}1.7$ kW. From the experiment, the deposition rate of a static state and a moving state were measured to be about 45 nm/min and 6 nm m/min at the distance of 50 mm between the target and the substrate, respectively.

• Journal of Korean Vacuum Science & Technology
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• v.2 no.2
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• pp.133-138
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• 1998

To enhance the ionization level of I-PVD and reduce the coil voltage two approaches were tried and as a diagnostic, optical emission spectroscopy and impedance analysis of the plasma was done with a range of Ar pressures and RF power along with XRD analysis of deposited Ag films. RF sputtering power was pulsed with various on/off time scales to recover the ICP quenched by sputtered metals. This in average enhances the ionization of the sputtered atoms with 10 ms/10 ms and 100 ms/100ms pulse on/off time duration and gives higher (200) preferred orientation over (111) in deposited Ag films. Secondly, Small axial B field about 8G remarkably reduced RF coil sputtering and showed scaled relationship between RF power and magnetic field strength for optimal process condition. From OES of Ar0 and Ar+, wave-like dispersion structure appeared and reduced the coil voltage about 20% at very weak field strength of 8G. This should be studied further to have nay relation with low mode helicon wave launching.

• 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

• 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).

• 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.