• 한국자기학회지
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• 제11권3호
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• pp.109-113
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• 2001

Presently, an inductor adapted at MMIC (Monolithic Microwave Integrated Circuit) which is used for cellular phone or PHS operates at quasi-microwave range over 800 MHz. However, a W-CDMA (Wideband Code Division Multiple Access) will use about 2 GHz range. Therefore magnetic film device should be compatible up to 2 GHz. We have deposited Co-Pd-Al-O system film using rf sputtering method which is expected up to 2 GHz, and investigated the effect of Pd content and magnetic field annealing. When Pd composition is 19%, Hk was 118 Oe, and ${\mu}$′showed flat frequency characteristics up to 1.5 GHz. The Q factor (=${\mu}$′/${\mu}$") was 23.3 at 1 GHz, 6.7 at 1.5 GHz and 1.5 at 2 GHz, respectively. Resonance frequency was 2 GHz. Therefore Co-Pd-Al-O thin film could be used at over 1 GHz, and also expected as an inductor material for wide band CDMA type cellular phone.

• E2M - 전기 전자와 첨단 소재
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• 제8권1호
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• pp.6-12
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• 1995

High Tc superconducting YBa$_{2}$Cu$_{3}$$O_{7-x}$ thin films were prepared on various substrates by off-axis rf magnetron sputtering method to examine the substrate effects on the film structure and its R-T characteristics. The SEM analysis showed that the surface morphology of the grown YBa$_{2}$Cu$_{3}$O.sub 7-x/, film has different characteristic structure with different substrate used. The film on (100) SrTiO$_{3}$ substrate has critical current density of 3*10$^{5}$ A/cm$^{2}$ at 77K under zero magnetic field. The X-ray diffraction measurements revealed that the films on (100) SrTiO$_{3}$ substrate have mixed a-axis and c-axis normal to the substrate surface and the films on (100) MgO and ZrO$_{2}$/sapphire substrates have c-axis normal orientation to the substrate surface. However, YBa$_{2}$Cu$_{3}$$O_{7-x}$ films on (100) sapphire substrates showed no preferential orientation.ion.

• 한국진공학회지
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• 제12권4호
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• pp.269-274
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• 2003

The electrical, optical and structural properties of ZnNiO thin _ films deposited on Si substrates using rf-magnetron sputtering method have been investigated before and after the thermal annealing processes. The crystallinity of the ZnNiO thin film become degraded with increasing the Ni contents. This is mainly because the lattice of the thin film was expanded due to the oxygen-deficient conditions. Concerning the electrical properties of the thin film, the carrier concentration increases ($6.81\times10^{14}\textrm{cm}^{-2}$) and Hall mobility decreases (36.3 $\textrm{cm}^2$/Vㆍs) with higher doping concentration of Ni. However, the carrier concentration and Hall mobility became low ($1.10\times10^{14}\textrm{cm}^2$ and high (209.6 $\textrm{cm}^2$/Vㆍs), respectively, after the thermal annealing process at $1000 ^{\circ}C$. We also observed a strong luminescene center peaking at 546 nm in photoluminescence spectra, which was caused by a deep level center in the ZnO band gap with oxygen deficient ZnNiO structure.

• Journal of Electrical Engineering and Technology
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• 제2권4호
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• pp.532-536
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• 2007

Carbon nanotube (CNT) properties, produced using a magnetic null discharge (MND) plasma production technology, were investigated. We firstly deposited the Fe layer 200 nm in thickness on Si substrate by the magnetic null discharge sputter method at the substrate temperature of $300도C$, and then prepared CNTs on the catalyst layer by using the magnetic null discharge (MND) based CVD method. CNTs were deposited in a gas mixture of CH4 and N2 at a total pressure of 1 Torr by the MND-CVD method. The substrate temperature and the RF power were $650^{\circ}C$ and 600W, respectively. The characterization data indicated that the proposed source could synthesize CNTs even under relatively severe conditions for the magnetic null discharge formation.

• 한국전기전자재료학회논문지
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• 제19권4호
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• pp.373-378
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• 2006

We report on plasma damage free-sputtering technologies for organic light emitting diodes (OLEDs), organic thin film transistor (OTFT) and flexible displays by using a box cathode sputtering (BCS) method. Specially designed BCS system has two facing targets generating high magnetic fields ideally entering and leaving the targets, perpendicularly. This target geometry allows the formation of high-density plasma between targets and enables us to realize plasma damage free sputtering on organic layer without protection layer against plasma. The OLED with Al cathode prepared by BCS shows electrical and optical characteristics comparable to OLED with thermally evaporated Mg-Ag cathode. It was found that OLED with Al cathode layer prepared by BCS has much lower leakage current density ($1{\times}10^{-5}\;mA/cm^2$ at -6 V) than that $(1{\times}10^{-2}{\sim}-10^0\;mA/cm^2)$ of OLED prepared by conventional DC sputtering system. This indicates that BCS technique is a promising electrode deposition method for substituting conventional thermal evaporation and DC/RF sputtering in fabrication process of organic based optoelectronics.

• 한국전기전자재료학회:학술대회논문집
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• 한국전기전자재료학회 2005년도 추계학술대회 논문집 Vol.18
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• pp.53-54
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• 2005

We report on plasma damage free-sputtering technologies for organic light emitting diodes (OLEDs), organic thin rim transistor (OTFT) and flexible displays by using a box cathode sputtering (BCS) method. Specially designed BCS system has two facing targets generating high magnetic fields ideally entering and leaving the targets, perpendicularly. This target geometry allows the formation of high-density plasma between targets and enables us to realize plasma damage free sputtering on organic layer without protection layer against plasma. The OLED with top cathode prepared by BCS shows electrical and optical characteristics comparable to OLED with thermally evaporated Mg-Ag cathode. It was found that TOLED with ITO or IZO top cathode layer prepared by BCS has much lower leakage current density ($1\times10^{-5}$ mA/cm2 at -6V) than that ($1\times10^{-1}\sim10^{\circ}mA/cm^2$)of OLED prepared by conventional DC sputtering system. This indicates that BCS technique is a promising electrode deposition method for substituting conventional thermal evaporation and dc/rf sputtering in fabrication process of organic based optoelectronics.

• E2M - 전기 전자와 첨단 소재
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• 제10권8호
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• pp.813-818
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• 1997

In this study the thin film air core and magnetic core inductors consisting of planar coil and/or CoNbZr amorphous magnetic layers on a Si substrate were fabricated as spiral type by using rf magnetron sputtering and wet etching methods. The etchant solution was achieved by iron chloride solution(17.5 mol%) mixed with HF (20 mol%) during 150 sec which etched Cu films and CoNbZr/Cu/CoNbZr multi-layer films. They were about 10${\mu}{\textrm}{m}$ of thickness and 10$\times$10 mm$^2$of size. The properties of thin film magnetic core inductor were 400 nH of Q value at 10 MHz and the resonance frequency was about 300 MHz.

• 한국자기학회지
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• 제6권5호
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• pp.317-322
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• 1996

RF magnetron reactive sputtering 법으로 Fe-Zr-N 박막을 제작하여 열처리 온도와 질소 분압의 변화에 따른 포화자화, 보자력, 고주파에서의 투자율 그리고 열적 안정성을 조사하였다. Fe-Zr-N 박막은 비정질과 결정질의 경계 조성인 $Fe_{72-78}Zr_{7-10}N_{15-18}$의 조성범위에서 연자성을 나타내었다. 이러한 박막은 포화자속밀도 1.55 T, 1 MHz에서의 실효 투자율은 3000 이상의 연자성을 나타내고 열처리 온도 $550^{\circ}C$ 까지도 실효투자율 2500 정도의 열적 안정성을 나타내었다. X-선 회절 분석 결과 열처리에 의해서 ZrN 미결정이 석출하여 $\alpha-Fe$ 결정 성장이 억제되어 우수한 연자기적 성질이 나타난다고 판단된다. 이때 $\alpha-Fe$ 입자 크기는 $40~50\AA$, ZrN의 입자 크기는 $10~15\AA$이었다.

• 한국재료학회지
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• 제9권8호
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• pp.831-836
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• 1999

RF 스퍼터링법으로 제작한 비정질 (Fe(sub)1-xCo(sub)x)(sub)89Zr11 자성박막의 자기특성을 Co농도에 따라 조사하였다. 130 Oe의 인가자기장중 190~20$0^{\circ}C$ 에서 10분간 2단 열처리를 행하였을때, 시편중 x=0.4의 박막은 높은 자왜를 나타냄에도 불구하고 0.25 Oe의 낮은 보자력 H(sub)c과, 8.7 MHz, 10 mOe의 여기자기장에서 측정된 미분투자율 $\mu$(sub)d는 280 정도로 가장 양호한 값을 나타내었다. 이와 같은 거동은 박막내 최적의 압축응력상태에서 야기된 자기이방성의 변화에 기인한다.

• 한국자기학회지
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• 제16권2호
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• pp.140-143
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• 2006

단결정 상태의 $CoFe_2O_4$ 박막을 rf magnetron sputtering 증착법을 이용하여 (100) MgO 기판 위에 성장시켰다. X선 회절기, Rutherford back-scattering 분석기와 고감도 주사전자현미경을 이용하여 측정한 결과 증착된 박막이 기판과 잘 정렬되어 성장한 것을 확인할 수 있었다. $600^{\circ}C$의 기판 온도에서 성장한 페라이트 박막은 약 200nm크기의 사각형 형태로 규칙적으로 분포되어 있음이 관찰되었다. 그러나 $700^{\circ}C$의 기판 온도에서 성장한 박막은 불규칙한 모양으로 이루어져 있었으며 30nm에서 150nm에 이르는 다양한 입자 크기를 보이고 있었다. 섭동자화기를 이용한 자기이력곡선 측정 결과 성장한 박막의 자화용이축이 기판과 수직하게 배열하는 것을 알 수 있었다. 또한 MgO 기판과 성장 박막과의 격자상수 차이로 인하여 기판과 수직한 방향의 보자력은 매우 큰 값을 나타내었다. 즉 평행한 방향의 보자력은 283 Oe이고 수직한 방향의 보자력은 6800 Oe였다. $700^{\circ}C$의 기판 온도에 서 성장한 페라이트 박막은 $600^{\circ}C$의 기판 온도에서 성장한 박막의 보자력 및 포화자화 값과 유사한 값을 보였으나 각형비는 급격하게 감소하였다.