• Journal of the Korean Vacuum Society
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• v.21 no.5
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• pp.242-248
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• 2012

Valence band of a vacuum-reduced $TiO_2$ (001) surface has been carefully examined using synchrotron x-ray photoelectron spectroscopy to investigate variation of the gap state upon oxidation and thermal diffusion of $Ti^{3+}$ interstitials from the bulk. We compare our results with that obtained from $TiO_2$ (110) and aim to address a crystal-face dependency in the oxidation and diffusion rates of $Ti^{3+}$ interstitials. We find very similar behaviors in the oxidation and thermal diffusion rate of $Ti^{3+}$ interstitials between the two crystal faces suggesting a negligible crystal-face dependency in this case.

• Korean Journal of Materials Research
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• v.27 no.11
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• pp.603-608
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• 2017

$Si_3N_4$ is a ceramic material attracting attention in many fields because of its excellent abrasion resistance. In addition, Ti and TiAl alloys are metals used in a variety of high temperature environments, and have attracted much attention because of their high strength and high melting points. Therefore, study of the interface reaction between $Si_3N_4/Ti$ and $Si_3N_4/TiAl$ can be a useful practice to identify phase selection and diffusion control. In this study, $Si_3N_4/Ti_5Si_3+TiN/TiN/Ti$ diffusing pairs were formed in the $Si_3N_4/Ti$ interfacial reaction and $Si_3N_4/TiN(Al)/Ti_3Al/TiAl$ diffusion pathway was identified in the $Si_3N_4/TiAl$ interfacial reaction. The diffusion layers of the interface reactions were identified and, to investigate the kinetics of the diffusion layer, the integrated diffusion coefficients were estimated.

• Proceedings of the KIEE Conference
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• 2001.11a
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• pp.9-11
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• 2001

차세대 고속 DRAM기술에 사용될 금속인 Cu의 확산 방지막(diffusion harrier) 물질로는 Ta 또는 W 같은 Refractory metal 이 융점(melting point)이 높고 저항값이 낮아 많이 연구 보고되고 있으나, 본 논문에서는 초고주파 소자에서 Au의 확산 방지 막으로 많이 사용되고 있으며. 선택적 증착이 용이한 Pt과 Ni를 MOS 소자의 Cu 확산 방지 막으로 적용하며 어닐링한 후 소자의 게이트 산화막 누설전류($I_{leak}$), 그리고. Si/$SiO_2$ 계면의 trap density 등의 변이를 측정하여 Cu가 소자의 특성 열화에 미치는 영향을 연구하였다. 실험 결과 Pt/Ti($200{\AA}/100{\AA}$)를 적용한 경우 소자 측성 열화가 가장 적었으며. 이는 Copper의 확산 방지막으로 Pt/Ti를 사용하여 전기적 특성 및 계면 특성을 개선시킬 수 있음을 보여 주었다. 이는 SIMS Profile을 통해서도 확인하였다.

• Journal of the Korean Vacuum Society
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• v.7 no.2
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• pp.112-117
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• 1998

TiN has been investigated as a good candidate for a diffusion barrier of Cu. Therefore, in this study, the grain boundary diffusion of Cu in TiN film was investigated by X-ray photoelectron spectroscopy(XPS). In general, TiN has a columnar grain structure. In the relatively lower temperature, less than 1/3 of the melting point, it was observed that Cu diffused into TiN mainly along the grain boundaries of TiN. The grain size of TiN was measured by atomic force microscope (AFM). In order to estimate the grain boundary diffusion constants, we used the modified surface accumulation method. The activation energy, $Q_b$ was 0.23 eV, and the diffusivity, $D_{bo}$ was $5.5\times10^{-12{\textrm{cm}^2$/sec.

• Korean Journal of Materials Research
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• v.5 no.2
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• pp.169-177
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• 1995

The diffusion barrier property of 100-nm-thick titanium nitride (TiN) film between Cu and Si was investigated using sheet resistance measurements, etch-pit observation, x-ray diffractometry, Auger electron spectroscopy, and transmission electron microscopy. The TiN barrier fails due to the formation of crystalline defects (dislocations) and precipitates (presumably Cu-silicides) in the Si substrate which result from the predominant in-diffusion of Cu through the TiN layer. In contrast with the case of Al, it is identified that the TiN barrier fails only the in-diffusion of Cu because there is no indication of Si pits in the Si substrate. In addition, it appears that the stuffing of TiN does not improve the diffusion barrier property in the Cu/TiN/Si structure. This indicates that in the case of Al, the chemical effect that impedes the diffusion of Al by the reaction of Al with $TiO_{2}$ which is present in the grain boundaries of TIN is very improtant. On the while, in the case of Cu, there is no chemical effect because Cu oxides, such as $Cu_{2}O$ or CuO, is thermodynamically unstable in comparison with $TiO_{2}$. For this reason, it is considered that the effect of stuffing of TiN on the diffusion barrier property is not significant in the Cu/ TiN/Si structure.

• Korean Journal of Materials Research
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• v.5 no.1
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• pp.87-95
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• 1995

The effect of stuffing of TiN on the diffusion barrier property between A1 and Si was investigated. The stuffing of TiN was performed by annealing in a Nz ambient at $450^{\circ}C$ for 30min. By TEM analysis, it is identified that there are solid-free or open spaces of a b u t 10-20$\AA$ between the grains of asdeposited TiN. In the case of stuffed TiN, the width of solid-free or open spaces has been reduced to about 10$\AA$ or below. The combination of RBS and AES analyses showed that the asdeposited TiN had about 7at.% of oxygen, and that the stuffed TiN had about 10-15at.% of oxygen. The diffusion barrier test result shows that after annealing at $650^{\circ}C$ for lhour, the asdeposited TiN fails due to the formation of A1 spikes and Si pits in the Si substrate. However, in the case of stuffed TiN, there is no indication of Al spikes and Si pits at the same annealing condition. Thus, it is concluded that this stuffing of TiN significantly improves the diffusion barrier property of TiN between A1 and Si. It is considered that the stuffing effect results from the reduced diffusion through grain boundaries due to the reduced spacing of grain boundaries.

• Journal of the Korean Institute of Telematics and Electronics D
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• v.36D no.5
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• pp.69-79
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• 1999

In this paper, we proposed a diffuion model of Ti diffused lithium niobate optical waveguide for fabricating waveguides with high refractive index and compared with conventional one. The achivement of low optical insertion loss between waveguide interface and single mode fibers was discussed as a function of Ti thickness for $\lambda$=1.55$\mu\textrm{m}$ The proposed diffusion method exhibited higher refractive index waveguide than conventional one for $\lambda$=0.6328$\mu\textrm{m}$ We have achieved the total fiber-waveguide-fiber insertion loss as low as 0.5dB/cm in z-cut and 1$\pm$0.5dB/cm in x-cut for both TM and TE mode of Mach-Zehnder interferometric waveguide in the range of Ti thickness 1000-1400$\AA$ for $\lambda$=1.55$\mu\textrm{m}$ From these results, this diffusion model for making a low loss waveguide can be used for low-power-modulators and switches.

• Proceedings of the Korean Vacuum Society Conference
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• 2011.02a
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• pp.179-179
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• 2011

관통전극(TSV, Trough Silicon Via) 기술은 전자부품의 소형화, 고성능화, 생산성 향상을 이룰 수 있는 기술이다. Cu는 현재 배선 기술에 적용되고 있고 전기적 저항이 낮아서 TSV filling 재료로 사용된다. 하지만 확산 방지막에 의해 완벽히 감싸지지 않는다면, Cu+은 빠르게 절연막을 통과하여 Si 웨이퍼로 확산된다. 이런 현상은 절연막의 누설과 소자의 오동작 등의 신뢰성 문제를 일으킬 수 있다. 현재 TSV의 제조와 열 및 기계적 응력에 관한 연구는 활발히 진행되고 있으나 Biased-Thermal Stress(BTS) 조건하의 Cu 확산에 관한 연구는 활발하지 않는 것이 실정이다. 이를 위해 본 연구에서는 TSV용 Cu 확산 방지막 Ti에 대해 Cu+의 drift 억제 특성을 조사하였다. 실험을 위해 Cu/확산 방지막/Thermal oxide/n-type Si의 평판 구조를 제작하였고 확산 방지막의 두께에 따른 영향을 조사하기 위해 Ti의 두께를 10 nm에서 100 nm까지 변화하였으며 기존 Cu 배선 공정에서 사용되는 확산 방지막 Ta와 비교하였다. 그리고 Cu+의 drift 측정을 위해 Biased-Thermal Stress 조건(Thermal stress: $275^{\circ}C$, Bias stress: +2MV/cm)에서 Capacitance 및 Timedependent dielectric breakdown(TDDB)를 측정하였다. 그 결과 Time-To Failure(TTF)를 이용하여 Cu+의 drift를 측정할 수 있었으며, 확산 방지막의 두께가 증가할수록 TTF가 증가하였고 물질에 따라 TTF가 변화하였다. 따라서 평판 구조를 이용한 본 실험의 Cu+의 drift 측정 방법은 향후 TSV 구조에서도 적용 가능한 방법으로 생각된다.

• Proceedings of the Korean Ceranic Society Conference
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• 2003.10a
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• pp.196.2-196
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• 2003

• Proceedings of the Korean Institute of Surface Engineering Conference
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• 2011.05a
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• pp.187-187
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• 2011

지르코니아 ($ZrO_2$) 표면에 금속 (Au)으로 표면 코팅한 후 Ti-6Al-4V와 진공 브레이징 접합을 행하였다. 표면에 코팅한 Au 층의 영향을 비교 분석하기 위하여 Au를 코팅하지 않은 지르코니아도 모재로 사용하였다. 접합소재로는 Ag-Cu-Ti계 active filler를 사용하였다. $ZrO_2$/Ti-6Al-4V 브레이징 결과, active filler는 양측 모재 표면에 wetting 되었으며, Ti-6Al-4V 내부로 filler 확산으로 인하여 두 모재의 direct joint가 관찰되었다. 접합 계면 사이에 접합부 결함은 관찰되지 않았다.