• Title/Summary/Keyword: Si-Al 배열상태

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Application of CBED Techniques of Energy Filtering TEM for Si-Al Disordering Study of Albite (알바이트의 Si-Al 배열상태 연구를 위한 에너지여과 투과전자현미경의 CBED법 적용)

  • Lee Young Boo;Kim Youn Joong;Lee Joung Hoo
    • Journal of the Mineralogical Society of Korea
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    • v.17 no.4
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    • pp.327-338
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    • 2004
  • XRD studies on annealed Na-feldspar (Amelia albite) at $1100^{\circ}C$ showed rapid structural changes due to Si-Al disordering, which resulted in phase transformations from low albite to high albite by 4-days annealing test. TEM SAED analyses on the annealed samples revealed a trend of structural changes, but estimation of the structural state was difficult due to a large deviation of the SAED data. Optimum conditions of CBED analyses on albite was established by employing a cooling specimen holder, 120 kV of acceleration voltage, 37 Jim of condenser aperture size and 25 nm of spot size. A proper orientation showing distinct changes of HOLZ lines corresponding to the structure changes of albite turned out to be close to the [418] direction with $-1.2^{\circ}$ tilting, where the width of two HOLZ lines in low albite was opposite to those in high albite.

XRD and TEM Investigations of Structures and Phase Transformations in Albite (XRD와 TEM을 이용한 알바이트의 구조 및 상전이 연구)

  • 김윤중;이영부
    • Journal of the Mineralogical Society of Korea
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    • v.16 no.1
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    • pp.91-106
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    • 2003
  • XRD results on annealing studies of Na-feldspars (Amelia albite) show rapid changes in the lattice parameters of the $1073^{\circ}C$-heated samples owing to disordering of Al and Si as well as lattice distortions upon quenching of the heated specimens. While a low albite transformed to a high albite by 7-days annealing at $1073^{\circ}C$, it remains as an early intermediate albite even by 140-days annealing at $924^{\circ}C$ due to the slower Al-Si disordering rate. From the heated samples tweed structures of $100∼200\AA$ were typically observed by TEM, which showed different ways of development between the $1073^{\circ}C$ -heated one and the $923 ^{\circ}C$ -heated one. The former locally trans-farmed to rnicrostructures similar to albite twin, while the latter transformed to domain structures containing albite twin plane in the wider area. The origin of tweed structures is suggested to be formation of incipient twins (albite twin and pericline twin) to reduce the lattice instability which is increased by disordering of Al and Si as well as quenching.

A Study on Microstructures and Chemistry of Anorthoclase Using Electron Microscopy (전자현미경을 이용한 Anorthoclase의 미세구조 및 화학 연구)

  • 이영부;김윤중;이석훈;이정후
    • Journal of the Mineralogical Society of Korea
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    • v.16 no.3
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    • pp.233-243
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    • 2003
  • Microstructures and chemistry of anorthoclase, a high-temperature phase of alkali feldspars, were studied using EPMA and TEM. BSE images of anorthoclase displayed mixtures of Na-rich areas and K-rich areas forming lamella of various sizes. EPMA analysis indicated that the Na-rich area is composed of Ab: 81%, Or: 3% and An: 11% in average, while the K-rich area is composed of Ab: 45%, Or: 44% and An: 11 % in average. TEM analysis revealed albite with Albite twins in the Na-rich area, contrasting to mixtures of albite with fine Albite twins and orthoclase without twins, forming regular lamella of about 100 nm sizes, in the K-rich area. The [001] electron diffraction pattern of the K-rich area also indicated coexistence of the two phases. While streaking parallel to the (010)$^{*}$ direction appeared only in albite due to the twin structure, streaking parallel to the $(100)^{ *}$ direction appeared both in albite and orthoclase, probably due to strain on the interface as well as order-disorder phenomena of Al and Si. It is suggested that the reverse orientation of albite and orthoclase is caused by pole switching to reduce strain on their interfaces. Based on these observations and analyses, the mineral studied is identified as lower-temperature cryptoperthite rather than high-temperature anorthoclase, which has a midium degree of Al-Si ordering and $400^{\circ}C$$600^{\circ}C$ of estimated temperatures for the microstructure formation.

Ellipsometric Study in Vacuum

  • Kim, Yeong-Dong
    • Proceedings of the Korean Vacuum Society Conference
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    • 2012.08a
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    • pp.63-63
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    • 2012
  • 편광분석법(ellipsometry)은 대상 물질의 유전율 함수의 실수부와 허수부를 Kramers-Kronig 관계식의 도움 없이 그 물질상수를 정확히 측정할 수 있는 매우 우수한 기술이다. 이 기술의 큰 장점 중 하나는 빛의 편광상태의 변화를 이용한 비파괴적인 방법으로써 실시간 측정이 가능하며, 박막의 두께측정의 오차범위는 0.1 nm 이하로써 매우 정확하다는 것이다. 본 연구자는 이러한 우수한 측정 기술인 편광분석법을 고진공의 분자살박막증착장치(MBE) 와 결합하여 AlSb, AlP의 유전율 함수를 측정하였다. Al 계열을 포함하는 반도체 화합물은 Al의 산소친화력이 강해 대기 중에서 순수한 유전율 함수를 얻기가 불가능하다. 하지만 본 연구실에서 초고진공 상태의 MBE 챔버에서 시료를 성장시키는 동시에 실시간으로 편광분석기를 이용하여 측정하였고, 지금까지 발표된 결과들 중 가장 순수한 상태의 AlSb 유전율 함수를 얻어낼 수 있었다. 또한 순수한 AlP의 유전함수를 측정할 수 있었고, 이는 편광분석기를 이용한 최초의 실험결과로써 이차미분을 이용한 전이점 분석결과 이론적인 전자밴드구조에서 E1, E1+${\Delta}1$, E2에 해당하는 밴드갭들을 확인할 수 있었다. 또한 표면의 원자배열 구조와 실시간으로 일어나는 그들의 역학적인 현상들에 관한 정보를 얻을 수 있는 surface photoabsorption (SPA)를 metalorganic chemical vapor deposition (MOCVD)에 장착하여 실시간 모니터링이 가능하도록 하였다. SPA를 이용하여 GaAs/AlGaAs 양자우물구조의 성장을 원자층 수준으로 실시간 모니터링을 할 수 있었다. 그리고 SPA를 이용하여 MOCVD 안에서 InP에 As가 흡착 및 탈착되는 현상을 분석하여, As의 흡착이 두 단계에 의해 이루어짐을 분석하였다. 그리고 편광분석법의 빠르고 정확한 측정 기술을 규칙적인 구조체에서 전자기파의 회절을 구할 수 있는 Rigorous Coupled-Wave Analysis (RCWA) 계산방법과 결합하여 나노구조의 기하학적인 모양을 정확하고 빠르게 구할 수 있었다. 본 연구를 위해 규칙적인 3차원 Si 구조체 제작하여 편광분석기로 측정하고 $SiO_2$와 표면 거칠기를 고려하여 RCWA로 분석한 결과, 규칙적인 Si 구조와 산화막 층까지 정확하게 분석할 수 있음을 확인하였다. 또한 규칙적인 나노구조분석 연구를 넘어 불규칙적인 나노구조에 대한 분석 가능성을 보이기 위해 InAs 양자점을 증착하여 분석하였고, 이를 통해 편광분석법과 RCWA를 이용하여 불규칙적인 나노구조의 모양과 크기, 분포의 분석이 가능함을 보였다.

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$1{times}8$ Array of GaAs/AlGaAs quantum well infrared photodetector with 7.8$\mu\textrm{m}$ peak response ($1{times}8$ 배열, 7.8 $\mu\textrm{m}$ 최대반응 GaAs/AlGaAs 양자우물 적외선 검출기)

  • 박은영;최정우;노삼규;최우석;박승한;조태희;홍성철;오병성;이승주
    • Korean Journal of Optics and Photonics
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    • v.9 no.6
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    • pp.428-432
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    • 1998
  • We fabricated 1$\times$8 array of GaAs/AlGaAs quantum well infrared photodetectors for the long wavelength infrared detection which is based on the bound-continuum intersubband transition, and characterized its electrical and optical properties. The device was grown on SI-GaAs(100) by the molecular beam epitaxy and consisted of 25 period of 40 ${\AA} $ GaAs well and 500 ${\AA} $ $Al_{0.28} Ga_{0.72}$ As barrier. To reduce the possibility of interface states only the center 20 ${\AA} $ of the well was doped with Si ($N_D=2{\times}10^{18} cm^{-3}$). We etched the sample to make square mesas of 200$\times$200 $\mu\textrm{m}^2$ and made an ohmic contact on each pixel with Au/Ge. Current-voltage characteristics and photoresponse spectrum of each detector reveal that the array was highly uniform and stable. The spectral responsivity and the detectivity $D^*$ were measured to be 180,260 V/W and $4.9{\times}10^9cm\sqrt{Hz}/W$ respectively at the peak wavelength of $\lambda$ =7.8 $\mu\textrm{m}$ and at T=10 K.

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Three Dimensional Finite Element Analysis of Particle Reinforced Metal Matirx Composites Considering the Thermal Residual Stress and the Non-uniform Distribution of Reinforcements (금속복합재료의 열잔류 응력과 강화재의 불규칙 분산 상태를 고려한 3차원 유한 요소 해석)

  • 강충길;오진건
    • Journal of the Korean Society for Precision Engineering
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    • v.17 no.6
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    • pp.199-209
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    • 2000
  • Particles reinforced MMCs have higher specific modulus, higher specific strength, better properties at elevated temperatures and better wear resistance than monolithic metals. But the coefficient of thermal expansion(CTE) of Al6061 is 5 times larger than that of SiCp. The discrepancy of CTE makes some residual stresses inside of MMCs. This work investigates Si$C_p$/Al6061 composites at high temperatures in the microscopic view by three-dimensional elasto-plastic finite element analyses and compares the analytical results with the experimental ones. The theoretical model is not able to consider the nonuniform shape of particle. So the shape of particle is assumed to be perfect global shape. And also particle distribution is not homogeneous in experimental specimen. It is assumed to be homogeneous in simulation model. The type of particle distribution is face-centered cubic array(FCC array). Furthermore, non-homogeneous distribution is modeled by combination of several volume fractions.

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Elastic Behavior of Zeolite Mesolite under Hydrostatic Pressure (제올라이트 메소라이트의 수압 하 탄성특성)

  • Lee, Yong-Jae;Lee, Yong-Moon;Seoung, Dong-Hoon;Jang, Young-Nam
    • Economic and Environmental Geology
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    • v.42 no.5
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    • pp.509-512
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    • 2009
  • Powder diffraction patterns of the zeolite mesolite ($Na_{5.33}Ca_{5.33}Al_{16}Si_{24}O_{80}{\cdot}21.33H_2O$), with a natrolite framework topology were measured as a function of pressure up to 5.0 GPa using a diamond-anvil cell and a $200{\mu}m$-focused monochromatic synchrotron X-ray. Under the hydrostatic conditions mediated by pore-penetrating alcohol and water mixture, the elastic behavior of mesolite is characterized by continuous volume expansion between ca. 0.5 and 1.5 GPa, which results from expansion in the ab-plane and contraction along the c-axis. Subsequent to this anomalous behavior, changes in the powder diffraction patterns suggest possible reentrant order-disorder transition. The ordered layers of sodium- and calcium-containing channels in a 1:2 ratio along the b-axis attribute to the $3b_{natrolite}$ cell below 1.5 GPa. When the volume expansion is completed above 1.5 GPa, such characteristic ordering reflections disappear and the $b_{natrolite}$ cell persists with marginal volume contraction up to ca. 2.5 GPa. Further increase in pressure leads to progressive volume contraction and appears to generate another set of superlattice reflections in the $3c_{natrolite}$ cell. This suggests that mesolite in the pressure-induced hydration state experiences order-disorder-order transition involving the motions of sodium and calcium cations either through cross-channel diffusion or within the respective channels.