• Title/Summary/Keyword: layer deposition

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Enhanced Adhesion of Cu Film on the Aluminum Oxide by Applying an Ion-beam-mixd Al Seed Layar

  • Kim, Hyeong-Jin;Park, Jae-Won
    • Proceedings of the Korean Vacuum Society Conference
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    • 2012.08a
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    • pp.229-229
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    • 2012
  • Adhesion of Copper film on the aluminum oxide layer formed by anodizing an aluminum plate was enhanced by applying ion beam mixing method. Forming an conductive metal layer on the insulating oxide surface without using adhesive epoxy bonds provide metal-PCB(Printed Circuit Board) better thermal conductivities, which are crucial for high power electric device working condition. IBM (Ion beam mixing) process consists of 3 steps; a preliminary deposition of an film, ion beam bombardment, and additional deposition of film with a proper thickness for the application. For the deposition of the films, e-beam evaporation method was used and 70 KeV N-ions were applied for the ion beam bombardment in this work. Adhesions of the interfaces measured by the adhesive tape test and the pull-off test showed an enhancement with the aid of IBM and the adhesion of the ion-beam-mixed films were commercially acceptable. The mixing feature of the atoms near the interface was studied by scanning electron microscopy, Auger electron spectroscopy, and X-ray photoelectron spectroscopy.

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Single-Domain-Like Graphene with ZnO-Stitching by Defect-Selective Atomic Layer Deposition

  • Kim, Hong-Beom;Park, Gyeong-Seon;Nguyen, Van Long;Seong, Myeong-Mo
    • Proceedings of the Korean Vacuum Society Conference
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    • 2016.02a
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    • pp.329-329
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    • 2016
  • Large-area graphene films produced by means of chemical vapor deposition (CVD) are polycrystalline and thus contain numerous grain boundaries that can greatly degrade their performance and produce inhomogeneous properties. A better grain boundary engineering in CVD graphene is essential to realize the full potential of graphene in large-scale applications. Here, we report a defect-selective atomic layer deposition (ALD) for stitching grain boundaries of CVD graphene with ZnO so as to increase the connectivity between grains. In the present ALD process, ZnO with hexagonal wurtzite structure was selectively grown mainly on the defect-rich grain boundaries to produce ZnO-stitched CVD graphene with well-connected grains. For the CVD graphene film after ZnO stitching, the inter-grain mobility is notably improved with only a little change in free carrier density. We also demonstrate how ZnO-stitched CVD graphene can be successfully integrated into wafer-scale arrays of top-gated field effect transistors on 4-inch Si and polymer substrates, revealing remarkable device-to-device uniformity.

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INVESTIGATION OF ENERGETIC DEPOSITION OF Au/Au (001) THIN FILMS BY COMPUTER SIMULATION

  • Zhang, Q. Y.;Pan, Z. Y.;Zhao, G. O.
    • Journal of the Korean Vacuum Society
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    • v.7 no.s1
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    • pp.183-189
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    • 1998
  • A new computer simulation method for film growth, the kinetic Monte Carlo simulation in combination with the results obtained from molecular dynamics simulation for the transient process induced by deposited atoms, was developed. The behavior of energetic atom in Au/Au(100) thin film deposition was investigated by the method. The atomistic mechanism of energetic atom deposition that led to the smoothness enhancement and the relationship between the role of transient process and film growth mechanism were discussed. We found that energetic atoms cannot affect the film growth mode in layer-by-layer at high temperature. However, at temperature of film growth in 3-dimensional mode and in quasi-two-dimensional mode, energetic atoms can enhance the smoothness of film surface. The enhancement of smoothness is caused by the transient mobility of energetic atoms and the suppression for the formation of 3-dimensional islands.

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Atomic Layer Deposition of $Sb_2S_3$ Thin Films on Mesoporous $TiO_2$

  • Han, Gyu-Seok;Jeong, Jin-Won;Seong, Myeong-Mo
    • Proceedings of the Korean Vacuum Society Conference
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    • 2013.02a
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    • pp.282-282
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    • 2013
  • The antimony sulfide ($Sb_2S_3$) thin films were deposited using the gas phase method which known as atomic layer deposition (ALD) on mesoporous micro-films. Tris (dimethylamido) antimony (III[$(Me_2N)_3Sb$] and hydrogensulfide ($H_2S$) were used as precursors to deposit $Sb_2S_3$. Self-terminating nature of $(Me_2N)_3Sb$ and $H_2S$ reaction were demonstrated by growth rate saturation versus precursors dosing time. Absorption spectra and extinction coefficient were investigated by UV-VIS spectroscopy. Scanning electron microscopic analysis and X-ray photoelectron spectroscopy (XPS) depth profile were employed to determine the conformal deposition.

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Fabrication of Low Loss Silica Slab Waveguide by Flame Hydrolysis Deposition (FHD 공정에 의한 저손실 실리카 슬랩 도파로 형성)

  • 심재기;김태홍;신장욱;박상호;김덕준;성희경
    • Journal of the Korean Ceramic Society
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    • v.37 no.6
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    • pp.524-529
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    • 2000
  • Silica slab wavegudie was fabricated on Si substrates by FHD for planar optical passive devices. The slab waveguide consists of lower clad and core layers, where core layer index is controlled by GeO2 addition. Doping of GeO2 in silica is difficult because of the low deposition density due to nonspherical particle generation in FHD process. Silica core particles deposited at various conditions such as flame temperature and substrate scanning were analyzed by SEM and TEM. As the flame temperature increased, the surface roughness of the core layer was decreased up to 3.6 nm after consolidation. Index difference and thickness of core of slab waveguide were 0.3%, 8$\mu\textrm{m}$ respectively. Measured optical loss at TE mode was <0.04 dB/cm at 1.3$\mu\textrm{m}$ and <0.06 dB/cm at 1.55$\mu\textrm{m}$.

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Study of a change of Surface roughness of sphere by adjustment of extrusion at fused deposition (FDM 장치에서 주사량 조정에 대한 구면체의 표면정도 변화에 관한 연구)

  • 전재억;권광진;정진서;김수광;김광희;하만경
    • Proceedings of the Korean Society of Precision Engineering Conference
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    • 1997.10a
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    • pp.1042-1046
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    • 1997
  • Fused deposition modelling(FDM) is a rapid prototyping(RP) process that fabricates part layer by layer by deposition of molten thennoplastic material extrude from a nozzle. RP system has many benefit. One of the benefit would be the ability to experiment with physical objects of any complexity in a relatively short period of time. But it has a matter of surface roughness and geometric accuracy. We research into a change of Surface roughness making the sphere by adjustment of extrusion in FDM.

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Characteristic Analysis of $Al_2$O$_3$Thin Films Grown by Atomic Layer Deposition (ALD법으로 성장시킨 $Al_2$O$_3$ 박막의 특성분석)

  • 성석재;김동진;배영호;이정희
    • Proceedings of the IEEK Conference
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    • 2001.06b
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    • pp.185-188
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    • 2001
  • In this study, $Al_2$O$_3$films have been deposited with Atomic Layer Deposition(ALD) for gate insulator for MPTMA and $H_2O$ at low temperature below 40$0^{\circ}C$ . Conventional methods of $Al_2$O$_3$thin film deposition have suffered from the poor step coverage due to reduction of device dimension and increasing contact/via hole aspect ratio. ALD is a self-limiting growth process with controlled surface reaction where the growth rate is only dependent on the number of growth cycle and the lattice parameter of materials. ALD growth process has many advantages including accurate thickness control, large area and large batch capability, good uniformity, and pinholes freeness.

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Investigation of Initiation of Electroless Ni-P and Ni-Cu-P deposition on pure iron

  • Yiyong, W-U;Kim, M.;S.C. Kwon
    • Proceedings of the Korean Institute of Surface Engineering Conference
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    • 2001.11a
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    • pp.10-10
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    • 2001
  • In this paper, initial depositing process of electroless Ni-Cu-P alloy was investigated by means of SEM, TEM and AES. The results show that the initial deposition is inhomogeneous and there exist different transition layers between different coatings and substrates, which are decided by the structures and compositions of the bath. For Ni-P binary alloy, its deposition takes place superiorly at grain boundary and on some grains with beneficial texture, the thickness of transition layer composed of Ni-Fe-P reaches 2000 angstrom. But during initiation of Ni-Cu-P trinary alloy, only at grain boundary is prIor to be deposited electrolessly, transited layer contains Ni-Fe-Cu-P and is decreased to about 500 angstrom. The structures of the films of Ni-P and Ni-Cu-P are crystalline at the initial depositing stage. The mechanisms of the process are put forward in this paper.

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NiAl Behavior at Plasma Spray Deposition

  • Orban, Radu L.;Lucaci, Mariana;Rosso, Mario;Grande, Marco Actis
    • Proceedings of the Korean Powder Metallurgy Institute Conference
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    • 2006.09a
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    • pp.692-693
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    • 2006
  • Behavior of stoichiometric and near-stoichiometric NiAl at plasma spray deposition, without and with a bond coat, for coating layers realization on a low alloyed steel substrate, has been investigated. In all variants, NiAl particle melting and subsequent welding at the impact with substrate were observed, forming a relatively compact and adherent coating layer with the NiAl stability maintaining - all assuring the coating layer oxidation and corrosion resistance. Good results from these points of view, also validated through corrosion tests, were obtained for 45:55 Ni:Al composition without a bond coat but adopting an Ar protective surrounding of plasma jet.

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Electrical properties of hafnium silicate deposited by atomic layer deposition as a function of annealing temperature (ALD 방법으로 증착된 Hf-silicate 박막의 열처리온도에 따른 전기적 특성)

  • Seo, Young-Sun;Kim, Nam-Hoon;Roh, Young-Han
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2007.11a
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    • pp.107-108
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    • 2007
  • In order to investigate the electrical properties of Hf-silicate as a function of annealing temperature, Hf-silicate deposited by atomic layer deposition (ALD) was studied. After Hf-silicate film deposition, annealing was proceeded at $500^{\circ}C\;and\;700^{\circ}C$. The hysteresis of C-V curves and trapping charge densities were decreased after annealing process. As annealing temperature became higher from $500^{\circ}C\;to\;700^{\circ}C$, the capacitance equivalent thickness (CET) was increased from 1.66 nm to 1.76 nm and the leakage current at -1 V was decreased from $1.70{\times}10^{-4}\;to\;5.68{\times}10^{-5}\;A/cm^2$.

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