• 한국신재생에너지학회:학술대회논문집
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• 2010.06a
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• pp.100.2-100.2
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• 2010

Superstrate형 실리콘 박막 태양전지에서 전면전극으로 사용되는 투명전도막의 표면형상은 태양전지내로 입사하는 태양광의 표면산란에 영향을 미치며 표면산란 증가를 통한 광 포획 및 단락전류밀도 향상을 통하여 태양전지 효율을 증대시키는 중요한 역할을 한다. 기존에 실리콘박막 태양전지용으로 많이 사용되는 상용 Asahi-U형 투명전도막은 수소 플라즈마에 대한 안정성이 낮고 입사광의 장파장 대역에서의 산란특성이 낮아 실리콘 박막 태양전지의 고효율화에 한계점이 있었다. 최근에 Asahi-U형 투명전도막을 대신하여 ZnO계 투명전도막을 전면전극으로 사용하려는 연구가 활발히 진행되고 있으며 Al을 토핑원소로 사용하는 ZnO:Al 투명전도막은 우수한 전기적, 광학적 특성과 수소플라즈마 안정성 및 저 비용 등의 우수한 장점을 갖고 있다. 스퍼터링 방식으로 제조된 ZnO:Al 투명전도막의 표면형상은 일반적으로 증착 후 습식식각을 통하여 조절되며 식각 전 박막의 미세구조에 영향을 받는 것으로 알려져 있다. 또한 습식 식각 이후의 표면거칠기에 따라 다양한 광학적, 전기적 특성을 나타낸다. 본 연구에서는 in-line RF-magnetron sputter 장비를 이용하여 다양한 공정조건하에서 ZnO:Al 투명전도막을 제조하고 증착된 박막의 미세구조 특성에 따른 습식식각 이후의 표면형상 변화 및 전기적 광학적 특성 변화를 조사하였다.

• Proceedings of the Korean Institute of Information and Commucation Sciences Conference
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• 2011.05a
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• pp.696-698
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• 2011

We present a new method for the fabrication of film bulk acoustic wave resonator (FBAR) devices that exploits the thin piezoelectric ZnO films particularly sputter-deposited in a mixture of N2O and Ar gases as the reactive and sputtering gases, respectively. Some thermal annealing treatments were performed on the as-deposited ZnO films and also their effects on the resonance characteristics of the FBAR devices were investigated. It was found that with an optimized process, the resonance characteristics of the fabricated FBAR devices could be further improved.

• Progress in Superconductivity
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• v.5 no.2
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• pp.105-108
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• 2004

We have studied effects of in-situ annealing on the fabrication of superconducting MgB$_2$ thin films prepared by rf magnetron co-sputtering. The Films were deposited on A1$_2$O$_3$ (1102) substrates at room temperature by using Mg and B targets. To trap remnant $O_2$ gas in the chamber, we used 20 mtorr Af sputter-gas balanced with 5 mol % of H$_2$ gas. To enhance adhesion to the substrate a thin layer of B was deposited prior to the codeposition of Mg and B. After completion of the film deposition, an additional Mg layer was deposited on top to compensate for Mg loss during the subsequent in-situ annealing. We have investigated the effects of two most important annealing parameters that are the Mg-to-B composition ratio and the annealing temperature. The range of the Mg-to-B composition ratio was from 0.42 to 0.85, and that of the annealing temperature was 500 $^{\circ}C$∼750 $^{\circ}C$. The Best result was obtained for the composition ratio of about 10% Mg excess from the stoichiometry and the annealing temperature of 700 $^{\circ}C$. Based on these results, we obtained films with T$_{c}$ : 36.5 K by further refining the fabrication process.s.

• Current Photovoltaic Research
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• v.3 no.3
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• pp.101-105
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• 2015

ZnO is gathering great interest for large square optoelectrical devices of flat panel display (FHD) and solar cell as a transparent conductive oxide (TCO). Herewith, Mg and IIIA (Al, In) co-doped ZnO films were prepared on SLG substrate using RF magnetron sputtering system. The effect of variation of atomic weight % of Mg and ZnO have been investigated. The atomic weight % Al and In are of 3% and kept constant throughout. The numbers of samples were prepared according to their different contents, which are $M_{3%}AZO_{94%}$, $M_{4%}AZO_{93%}-(MAZO)$ and $M_{3%}IZO_{94%}$, $M_{4%}IZO_{93%}-(MIZO)$ respectively. A RF power of 225 W and working pressure of 6 m Torr was used for the deposition at $300^{\circ}C$. All of the two thin film show good uniformity in field emission scanning electron microscopy image. $M_{3%}AZO_{94%}$ thin film shows overall better performance among the all. The film shows the best lowest resistivity, carrier concentration, mobility and Sheet resistance and is found to be are of $8.16{\times}10^{-4}{\Omega}cm$, $4.372{\times}10^{20}/cm^3$, $17.5cm^2/vs$ and $8.9{\Omega}/sq$ respectively. Also $M_{3%}AZO_{94%}$ thin film shows the relatively high optical band gap energy of 3.7 eV with high transmittance more than 80% in visible region required for the better solar cell performance.

• Korean Journal of Materials Research
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• v.21 no.6
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• pp.341-346
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• 2011

In this study, we inserted a Zn buffer layer into a AZO/p-type a-si:H layer interface in order to lower the contact resistance of the interface. For the Zn layer, the deposition was conducted at 5 nm, 7 nm and 10 nm using the rf-magnetron sputtering method. The results were compared to that of the AZO film to discuss the possibility of the Zn layer being used as a transparent conductive oxide thin film for application in the silicon heterojunction solar cell. We used the rf-magnetron sputtering method to fabricate Al 2 wt.% of Al-doped ZnO (AZO) film as a transparent conductive oxide (TCO). We analyzed the electro-optical properties of the ZnO as well as the interface properties of the AZO/p-type a-Si:H layer. After inserting a buffer layer into the AZO/p-type a-Si:H layers to enhance the interface properties, we measured the contact resistance of the layers using a CTLM (circular transmission line model) pattern, the depth profile of the layers using AES (auger electron spectroscopy), and the changes in the properties of the AZO thin film through heat treatment. We investigated the effects of the interface properties of the AZO/p-type a-Si:H layer on the characteristics of silicon heterojunction solar cells and the way to improve the interface properties. When depositing AZO thin film on a-Si layer, oxygen atoms are diffused from the AZO thin film towards the a-Si layer. Thus, the characteristics of the solar cells deteriorate due to the created oxide film. While a diffusion of Zn occurs toward the a-Si in the case of AZO used as TCO, the diffusion of In occurs toward a-Si in the case of ITO used as TCO.

• Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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• 2007.06a
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• pp.430-430
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• 2007

In this study, the nematic liquid crystal (NLC) alignment effects treated on the ZnO thin film layers using ion beam irradiation were successfully studied for the first time. The ZnO thin films were deposited on indium-tin-oxide (ITO) coated glass substrates by rf-sputter and The ZnO thin films were deposited at the three kinds of rf power. The used DuoPIGatron type ion beam system, which can be advantageous in a large area with high density plasma generation. The ion beam parameters were as follows: energy of 1800 eV, exposure time of 1 min and ion beam current of $4\;mA/cm^2$ at exposure angles of $15^{\circ}$, $30^{\circ}$, $45^{\circ}$, and $60^{\circ}$. The homogeneous and homeotropic LC aligning capabilities treated on the ZnO thin film surface with ion beam exposure of $45^{\circ}$ for 1 min can be achieved. The low pretilt angle for a NLC treated on the ZnO thin film surface with ion beam irradiation for all incident angles was measured. The good LC alignment treated on the ZnO thin film with ion beam exposure at rf power of 150 W can be measure. For identifying surfaces topography of the ZnO thin films, atomic force microscopy (AFM) was introduced. After ion beam irradiation, test samples were fabricated in an anti-parallel configuration with a cell gap of $60{\mu}m$.

• Journal of IKEEE
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• v.26 no.2
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• pp.232-239
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• 2022

We analyzed the effect of post-annealing on lithium phosphate (Li₃PO₄) solid-state thin-film. Li₃PO₄ thin films were deposited by radio frequency (RF) sputtering, with subsequent annealing of the films at 200-400 ℃. SEM imaging of the sample surfaces showed no significant difference in morphology between the annealed and non-annealed samples. XRD analysis indicated that the samples consist of an amorphous-like structure. Post-annealing changes in binding energy were confirmed by XPS analysis, while the leakage current density at -6 V was measured to be about 7.15 times lower in a device that had been annealed at 400 ℃ vs a non-annealed device. It was confirmed that the leakage current decreased with increasing post-annealing temperature.

• Proceedings of the KIEE Conference
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• 2001.11a
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• pp.103-105
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• 2001

ZnO thin films on glass substrate were deposited by RF sputter with various $Ar/O_2$ gas ratio. Crystallinities, surface morphologies, and electrical properties of the films were investigated by XRD(x-ray diffractometer), and SEM (scanning electron microscopy) analyses. The facing targets sputtering system can deposit thin film at plasma free condition and change the deposition condition in wide range. We suggested that a very suitable $Ar/O_2$ gas of ratio should be 50/50 for preparation of high quality ZnO films with good C-axis orientation.

• JSTS:Journal of Semiconductor Technology and Science
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• v.16 no.2
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• pp.210-214
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• 2016

In this paper, the decrease in the contact resistance of Ni germanide/Ge contact was studied as a function of the thickness of the antimony (Sb) interlayer for high performance Ge MOSFETs. Sb layers with various thickness of 2, 5, 8 and 12 nm were deposited by RF-Magnetron sputter on n-type Ge on Si wafers, followed by in situ deposition of 15nm-thick Ni film. The contact resistance of samples with the Sb interlayer was lower than that of the reference sample without the Sb interlayer. We found that the Sb interlayer can lower the contact resistance of Ni germanide/Ge contact but the reduction of contact resistance becomes saturated as the Sb interlayer thickness increases. The proposed method is useful for high performance n-channel Ge MOSFETs.

• Journal of the Korean Ceramic Society
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• v.46 no.1
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• pp.10-15
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• 2009

We have fabricated silicon-rich silica thin films via RF magnetron sputtering using a SiO target. Thickness evolution and microstructure change of such $SiO_x$ (1$SiO_x$ thin films turned out to be mainly responsible for the increase of refractive index.