• 한국진공학회:학술대회논문집
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• 한국진공학회 2009년도 제38회 동계학술대회 초록집
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• pp.383-383
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• 2010

Gas-phase hydrogen atoms create a variety of chemical and physical phenomena on Si surfaces: adsorption, abstraction of pre-adsorbed H, Si etching, Si amorphization, and penetration into the bulk lattice. Thermal desorption/evolution analyses exhibited three distinct peaks, including one from the crystalline bulk. It was previously found that thermal-energy gaseous H(g) atoms penetrate into the Si(100) crystalline bulk within a narrow substrate temperature window(centered at ~460K) and remain trapped in the bulk lattice before evolving out at a temperature as high as ~900K. Developing and sustaining atomic-scale surface roughness, by H-induced silicon etching, is a prerequisite for H absorption and determines the $T_s$ windows. Issues on the H(g) absorption to be further clarified are: (1) the role of the detailed atomic surface structure, together with other experimental conditions, (2) the particular physical lattice sites occupied by, and (3) the chemical nature of, absorbed H(g) atoms. This work has investigated and compared the thermal H(g) atom absorptivity of Si(100), Si(111) and Si(110) samples in detail by using the temperature programmed desorption mass spectrometry (TPD-MS). Due to the differences in the atomic structures of, and in the facility of creating atom-scale etch pits on, Si(100), (100) and (110) surfaces, the H-absorption efficiency was found to be larger in the order of Si(100) > Si(111) > Si(110) with a relative ratio of 1 : 0.22 : 0.045. This intriguing result was interpreted in terms of the atomic-scale surface roughening and kinetic competition among H(g) adsorption, H(a)-by-H(g) abstraction, $SiH_3(a)$-by-H(g) etching, and H(g) penetraion into the crystalline silicon bulk.

• 한국세라믹학회지
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• 제31권8호
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• pp.886-892
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• 1994

Structural and electrical properties of BaTiO3 thin films deposited on Pt/SiO2/Si substrates by RF magnetron sputtering method have been investigated. Crystallization behavior and electrical properties were studied for the films deposited under various sputtering gas compositions (Ar+O2 gas mixture) and substrate temperatures. All the films deposited above 50$0^{\circ}C$ were all crystallized and their preferred orientation changed from (001) to (111) with the addition of oxygen gas. The dielectric constant of films deposited in pure argon was about 110 and showed little dependence on the substrate temperature. But that was increased as the ratio of O2/Ar increased and its substrate temperature dependence was discernible. The highest dielectric constant reached to 550. In addition, the films deposited in mixed gas showed stable dielectric properties against the frequency and temperature.

• 한국전기전자재료학회:학술대회논문집
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• 한국전기전자재료학회 2006년도 하계학술대회 논문집 Vol.7
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• pp.18-19
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• 2006

The bismuth zinc niobate(BZN) pyrochlore thin films were fabricated on Pt(111)/Ti/$SiO_2$/p-Si(100) substrates using a reactive rf magnetron sputtering method at the conditions of working gas ratio Ar:$O_2$=90:10, substrate temperate $R.T{\sim}600^{\circ}C$, rf power 50 W. The dielectric constant, tunability, leakage current density and crystallinity of thin films changed with a substrate temperate. The BZN pyrochlore thin films sputtered with a substrate temperature of $600^{\circ}C$ and RTA at $800^{\circ}C$ showed a leakage current density lower than $10^{-8}\;A/cm^2$ at the range of ${\pm}300\;kV/cm$.

• 한국전기전자재료학회논문지
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• 제14권5호
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• pp.410-416
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• 2001

KLN thin films were fabricated on Pt coated Si(100) wafer using an rf-magnetron sputtering method. The grown KLN thin film consists of 4-fold grains. In this experiment, the structure of 4-fold grained thin film was investigated using XRD and SEM measurements. Pt layer was also deposited using the rf-magnetron sputtering method,. XRD measurement showed that he Pt thin film has Gaussian distribution form with strong (111) direction orientation. The KLN thin film has preferred-orientation of (001) direction, and the peak consists of 2 separate peaks; one with broad FWHM and the other with narrow FWHM. The sharp peak is due to single crystal, and combining with Em results, the 4-fold grain consists of singel crystals with c-axis normal to substrate.

• 한국진공학회:학술대회논문집
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• 한국진공학회 2002년도 제22회 학술발표회 초록집
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• pp.111-112
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• 2002

• 한국결정성장학회지
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• 제19권4호
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• pp.159-164
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• 2009

실리콘 기판에 GaN 에피성장을 확인하기 위해, P형 Si(100), Si(111) 기판 전면에 버퍼층으로 40 nm 두께의 코발트실리사이드를 형성시켰다. 형성된 코발트실리사이드 층에 연속으로 HVPE(hydride vapor phase epitaxy)로 하나는 $850^{\circ}C$-12분 + $1080^{\circ}C$-30분(공정I)과, 또 하나 조건은 $557^{\circ}C$-5분 + $900^{\circ}C$-5분(공정II) 조건으로 각각 나누어 진행하여 보았다. GaN의 에피성장을 광학현미경, 주사전자현미경, 주사탐침현미경, 그리고 HR-XRD로 확인하였다. 공정I로는 GaN의 에피성장이 진행되지 않았으며, 공정II에서는 에피성장이 진행되었다. 특히 공정 II는 열팽창에 의해 실리콘 기판과의 자가정렬적인 기판분리 현상을 보였으며, XRD로 GaN의 0002 방향의 결정성 (crystallinity)을 ${\omega}$-scan으로 확인한 결과(100)면 방향의\ 실리콘과 코발트실리사이드를 버퍼층으로 활용하고 저온에서 HVPE를 진행한 조합이 GaN의 에피성장에 유리하였다.

• 한국진공학회:학술대회논문집
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• 한국진공학회 2003년도 제24회 학술발표회 초록집
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• pp.168-168
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• 2003

• 한국진공학회:학술대회논문집
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• 한국진공학회 2009년도 제38회 동계학술대회 초록집
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• pp.59-59
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• 2010

Graphene is a 2-D sheet of $sp^2$-bonded carbon arranged in a honeycomb lattice. This material has attracted major interest, and there are many ongoing efforts in developing graphene devices because of its high charge mobility and crystal quality. Therefore clear understanding of the substrate effect and mechanism of synthesis of graphene is important for potential applications and device fabrication of graphene. In a published paper in J. Phys. Chem. C (2008), the effect of substrate on the atomic/electronic structures of graphene is negligible for graphene made by mechanical cleavage. However, nobody shows the interaction between Ni substrate and graphene. Therefore, we have studied this interaction. In order to studying these effect between graphene and Ni substrate, We have observed graphene synthesized on Ni substrate and graphene transferred on $SiO_2$/Si substrate through Raman spectroscopy. Because Raman spectroscopy has historically been used to probe structural and electronic characteristics of graphite materials, providing useful information on the defects (D-band), in-plane vibration of sp2 carbon atoms (G-band), as well as the stacking orders (2D-band), we selected this as analysis tool. In our study, we could not observe the doping effect between graphene and Ni substrate or between graphene and $SiO_2$/Si substrate because the shift of G band in Raman spectrum was not occurred by charge transfer. We could noticed that the bonding force between graphene and Ni substrate is more strong than Van de Waals force which is the interaction between graphene and $SiO_2$/Si. Furthermore, the synthesized graphene on Ni substrate was in compressive strain. This phenomenon was observed by 2D band blue-shift in Raman spectrum. And, we consider that the graphene is incommensurate growth with Ni polycrystalline substrate.

• 한국세라믹학회지
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• 제50권1호
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• pp.43-49
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• 2013

${\beta}$-SiC was deposited onto a graphite substrate by a LPCVD method and the effect of the crystallographic orientation on mechanical properties of the deposited SiC was investigated. The deposition was performed at $1300^{\circ}C$ in a cylindrical hot-wall LPCVD system by varying the deposition pressure and total flow rate. The texture and crystallographic orientation of the SiC were evaluated by XRD. The deposition rate increased linearly with the gas flow rate from 800 sccm to 1600 sccm. It also increased with the pressure but became saturated above a total pressure of 3.3 kPa. In the range of 3.3 - 10 kPa, the preferred orientation changed from the (220) and (311) planes to the (111) plane. The hardness and elastic modulus showed maximum values when the SiC had the (111) preferred orientation, though it gradually decreased upon a change to the (220) and (311) preferred orientations.

• 한국결정성장학회지
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• 제1권1호
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• pp.51-59
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• 1991

GaAs를 Si 웨이퍼에 성장시킬 때 초기단계의 핵생성에 대하여 computer simulation을 통해 이론적으로 고찰하였다. 기존의 핵생성이론과는 달리 초기의 미세한 핵의 경우 핵을 구성하는 ledge와 ledge간의 상호작용은 핵의 크기 및 모양에 의하여 결정되는 ledge간의 거리에 따라 변화함을 알 수 있었다. 따라서 여러 형태의 핵에 대하여 분석하여 본 결과 다층의 피라미드 형태로 GaAs 핵이 생성될 때 가장 낮은 excess에너지가 요구되었고 이와 같은 결과는 이러한 형태가 필연적으로 포함하게 되는 에너지가 낮은 Ga(111) facet 때문인 것으로 밝혀졌다. 그러므로 GaAs/Si에서 가장 문제가 되고 있는 전위결함도 초기의 핵생성에 크게 기인함을 알 수 있다.