• 제목/요약/키워드: lattice distortion

검색결과 97건 처리시간 0.021초

Effect of pH on the Luminescence of $(Y,Gd)BO_3:Eu^{3+}$ Phosphor Prepared by the Coprecipitation Method

  • Lee, Gwan-Hyoung;Kang, Shin-Hoo
    • 한국정보디스플레이학회:학술대회논문집
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    • 한국정보디스플레이학회 2005년도 International Meeting on Information Displayvol.II
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    • pp.1514-1517
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    • 2005
  • The $(Y,Gd)BO_3:Eu^{3+}$ phosphor was made by coprecipitation method. The precipitated powders were amorphous. The value of pH in the process of coprecipitation was critical for the luminescence of phosphors. The particle size and morphology were influenced by pH value. The lower calcination temperature and hydrothermal synthesis leads to the distortion of lattices. The distorted lattices changed the symmetry of $Eu^{3+}$ site. The broken inversion symmetry in the distorted lattice caused the increased emission of $^5D_0{\rightarrow}^7D_2$ transition.

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Finding interstitial oxygen in an Si substrate during low temperature plasma oxidation

  • Kim, Bo-Hyun;Ahn, Jin-Hyung;Ahn, Byung-Tae
    • 한국정보디스플레이학회:학술대회논문집
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    • 한국정보디스플레이학회 2003년도 International Meeting on Information Display
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    • pp.690-693
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    • 2003
  • An Si substrate (100) was oxidized at $400^{\circ}C$ in inductively coupled oxygen plasma. Interstitial oxygen was found in the Si substrate at the initial stage of oxidation by IR measurements. An x-ray rocking curve of Si substrates showed a lower peak intensity due to lattice distortion by the interstitial oxygen. The refractive index of thin oxides, below which interstitial oxygen existed in the Si substrate, was smaller than the refractive index of thick oxides, below which no interstitial oxygen existed. The interstitial oxygen was found by plasma oxidation using $O_{2}$ gas and $N_{2}O$ gas. The inductively coupled plasma oxidation using $N_{2}O$ gas was performed by atomic oxygen, not by molecular oxygen, indicating that atomic oxygen in plasma is responsible for the incorporation of interstitial oxygen.

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의사이성분계, Li2Cr2O4-MgCr2O4와 Li2Cr2O4-MgAl2O4에서의 LiCrO2 고용체 형성과 결합구조 (Solid Solution and Defect Structure of LiCrO2 in the Pseudo-binary Systems : Li2Cr2O4-MgAl2O4)

  • 정영서;오근호;김호기
    • 한국세라믹학회지
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    • 제25권1호
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    • pp.35-41
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    • 1988
  • In the system of Li2O-MgO-Al2O3-Cr2O3, the crystalline solid solution of LiCrO2 along the pseudo-binary join between rocksalt structure(LiCrO2) and spinel structure(MgCr2O4 or MgAl2O4) have been investigated by x-ray diffraction techniques. In this study, order-disorder phase transition of LiCrO2 was observed and the unit cell of the disordered LiCrO2 structure has been established. It has been found that LiCrO2 makes a solid solution over a wide range with MgAl2O4, while not with MgCr2O4. This difference was explained as being due to the ability of oxygen lattice distortion which depended on the relative sizes and chemical bonding characteristics of the substituted ions.

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가변 전송 Frame 길이를 갖는 저 전송속도 VQ 음성부호화 알고리즘에 대한 연구 (A Low Rate VQ Speech Coding Algorithm with Variable Transmission Frame Length)

  • 좌정우;이성로;이황수
    • The Journal of the Acoustical Society of Korea
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    • 제12권1E호
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    • pp.32-38
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    • 1993
  • 본 논문에서는 저 전송속도의 음성 부호화기를 제안하였고 컴퓨터 시뮬레이션을 통하여 성능분석과 유연성을 입증하였다. 제안된 부호화 방식은 입력 음성신호의 Stationarity에 따라 전송 프레임의 길이를 가변하고, 전송 프레임의 대표적인 특징 벡터를 Vector Quatization으로 부호화하였다. 제안된 부호화 방식에서 특징 벡터열은 입력 음성신호를 샘플단위로 Prewindowed RLS Lattice 알고리즘을 통해 구한 PARCOR 계수로 구성된다. 입력 음성신호는 Subsegment로 분할되고, 각 Subsegment에서 대표적인 PARCOR 계수를 구한다. Likelihood Ratio Distortion Measure를 사용하여 유사도에 따라 Subsegment를 병합함으로써 전송프레임을 결정한다. 컴퓨터 시뮬레이션 결과로부터 제안된 VTEL 음성 부호화 방식은 좋은 음질을 유지하면서 전체 전송속도를 크게 줄일 수 있다.

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HRTEM Study of Phase Transformation from Anatase to Rutile in Nanocrystalline $TiO_2$ Particles

  • Kim, Kyou-Hyun;Park, Hoon;Ahn, Jae-Pyoung;Lee, Jae-Chul;Park, Jong-Ku
    • 한국분말야금학회:학술대회논문집
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    • 한국분말야금학회 2006년도 Extended Abstracts of 2006 POWDER METALLURGY World Congress Part 1
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    • pp.466-467
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    • 2006
  • The anatase particle was facetted at the free surface and a neck formation between the anatase particles prior to the phase transformation occured. This resulted in the severe lattice distortion at the region of the interface near the neck and this can act as the nucleation sites for the phase transformation. The grain growth of rutile particles after the phase transformation grew very fast by the sweeping phenomena of grain boundary. Therfore, It leaded to the microstructure without the rutile phase located in anatase particle.

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The LS$\rightarrow$HS Transition of Cobalt(III) in an Oxygen Lattice with the $K_2NiF_4$-Type Structure: Correlations with the Chemical Bonding Environment of the $(CoO_6)$ Octahedron Along the c-axis

  • Byeon, Song-Ho;Demazeau, Gerard
    • Bulletin of the Korean Chemical Society
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    • 제15권11호
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    • pp.949-953
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    • 1994
  • In oxides characterized by the $K_2NiF_4-type$ structure, the low-spin${\to}$high-spin transition of trivalent cobalt ion was studied in function of the nature of competing bonds in the perovskite-plane and along the c-axis. Using Slichter and Drickamer's model the calculated values of parameters characterizing such a transition are correlated with the covalency of competing bonds along the c-axis of the $K_2NiF_4$-structure and the local structural distortion of the $(CoO_6)$ octahedron.

Correlation between Structures and Magnetism in Iron: Ferromagnetism and Antiferromagnetism

  • Lee, Dong-Kook;Hong, Soon-Cheol
    • Journal of Magnetics
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    • 제12권2호
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    • pp.68-71
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    • 2007
  • Even a pure bulk Fe has a complicated magnetic phase and its magnetism is still needed to be clarified. In this study we investigated the magnetism of bcc and fcc bulk Fe with total energy calculations as functions of atomic volume. The full-potential linearized augmented plane wave method was adopted within a generalized gradient approximation. The ground state of bulk Fe is confirmed to be of ferromagnetic (FM) bcc. For fcc structured Fe an antiferromagnetic (AFM) state is more stable compared to FM states which exist as low spin and high spin states. The stable AFM states were found to accompany a tetragonal distortion, while the FM states remained in a cubic symmetry. At an expanded lattice constant a high spin FM state was calculated to be able to be stabilized with significant enhanced magnetic moment compared to the value of the ground state, bcc FM.

첨가제(Y, Nb)에 따른 PTCR $BaTiO_3$계 세라믹스의 결정구조 해석과 상전이 특성 (Phase transition and crystal structure analysis of PTCR $BaTiO_3$ ceramics with dopants (Y, Nb))

  • 차용원;원승신;백종후;이희수;엄우식;송준광;이인식;정훈택
    • 한국결정성장학회지
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    • 제7권2호
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    • pp.253-258
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    • 1997
  • 반도체화 첨가제인 $Y_2O_3$$Nb_2O_5$ 첨가랑 변화에 따른 PTCR $BaTiO_3$ 세라믹스의 결정구조 해석과 상전이 특성을 연구하기 위하여 ($Ba_{0.85}Ca_{0.15})TiO_3$ + X m/o $Nb_2O_5$(Y m/o $Y_2O_3$) + 0.08 w/o $Mn(NO_3)_2$$6H_2O$ + 0.25 w/o $SiO_2$ 계에서 X는 0.1 ~ 0.4로 Y는 0.2 ~ 0.4로 각각 변화시켜 실험을 수행하였다. $Nb_2O_5$의 첨가시 B-site 치환에 따라서 격자상수가 선형적으로 변화하다가 0.3 mol% 이상 치환할 경우 c 축의 격자상수가 급격히 감소함을 알 수 있었다. 이는 octahedron distortion둥의 원인으로 판단되며, 이러한 격자상수 변화는 상전이 온도 결과와도 잘 일치함을 확인할 수 있었다. 또한 $Y_2O_3$ 첨가의 경우 0.3 mol%가지는 A, B-site를 각각 치환하며 그 이상부터는 A-site 이온을 주로 치환하는 것을 격자상수 변화와 상전이 온도결과를 통해 알 수 있었으며, Rietveld 해석결과 $Y^{3+}$가 A-site 치환시 $Ba^{2+}$$Ca^{2+}$를 같은 비율로 치환한다는 것을 알 수 있었다.

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원자층 증착법 기반 양이온-음이온 이중 도핑 효과에 따른 ZnO 박막의 전기적 특성 비교 연구 (An Investigation of Electrical Properties in Cation-anion Codoped ZnO by Atomic Layer Deposition)

  • 김동은;김건우;강경문;;박형호
    • 마이크로전자및패키징학회지
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    • 제30권3호
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    • pp.94-101
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    • 2023
  • 투명 전도성 산화물(TCO)를 대체할 수 있는 대표적인 물질로 알려진 ZnO는 3.37 eV의 bandgap과 60 meV의 exciton binding energy를 가진 반도체 물질이다. 본 연구에서는 투명 전극으로 사용하기 위한 높은 전기적 특성을 확보하기 위해 원자층 증착법을 기반으로 양이온과 음이온의 단일 및 이중 도핑에 따라 성장한 ZnO 박막을 제작하였다. 3가 양이온 Al, Ga과 음이온 F이 단일 및 이중 도핑된 ZnO 박막의 구조적, 광학적 특성 및 전기적 특성을 확인하였다. 단일 도핑의 경우, ZnO에 donor로 작용하는 Al, Ga, F에 의해 캐리어 농도가 도핑 전에 비해 증가하였고 근자외선 영역에서의 band-edge absorption이 증가하는 것을 확인하였다. 단일 도핑 중에서는 F이 ZnO 내 산소 공공 자리에 passivation 되면서 높은 mobility와 함께 가장 높은 전도도를 보였다. 이중 도핑의 경우, 각 원소들의 도핑 효과가 더해지면서 단일 도핑에 비해 높은 전기적 특성을 보였다. 결과적으로 Ga-F에 비해 Al-F 도핑 시 ionic radius 차이에 의한 lattice distortion 감소 및 delocalized 된 전자 상태의 증가로 가장 낮은 비저항 값을 보였으며 PDOS 분석을 통한 시뮬레이션 데이터로 측정 값과 일치하는 결과를 확인했다.

Effects of electron beam irradiation on the superconducting properties of YBCO thin films

  • Lee, Y.J.;Choi, J.H.;Jun, B.H.;Joo, J.;Kim, C.S.;Kim, C.J.
    • 한국초전도ㆍ저온공학회논문지
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    • 제18권4호
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    • pp.15-20
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    • 2016
  • The effects of electron beam (EB) irradiation on the superconducting critical temperature ($T_c$) and critical current density ($J_c$) of YBCO films were studied. The YBCO thin films were irradiated using a KAERI EB accelerator with an energy of 0.2 MeV and a dose of $10^{15}-10^{16}e/cm^2$. A small $T_c$ decrease and a broad superconducting transition were observed as the EB dose increased. The value of $J_cs$ (at 20 K, 50 K and 70 K) increased at doses of $7.5{\times}10^{15}$ and $2.2{\times}10^{16}e/cm^2$. However, $J_cs$ decreased as the dose increased further. The X-ray diffraction (XRD) analysis showed that the c axis of YBCO was elongated and the full width at half maximum (FWHM) increased as the dose increased, which is strong evidence of the atomic displacement by EB irradiation. The transmission electron microscopy (TEM) showed that the amorphous layer formed in the vicinity of the surfaces of the irradiated films. The amorphous phase was often present as an isolated form in the interior of the films. In addition to the formation of the amorphous phase, many striations running along the a-b direction of YBCO were observed. The high magnification lattice image showed that the striations were stacking faults. The enhancement of $J_c$ by EB irradiation is likely to be due to the lattice distortion and the formation of defects such as vacancies and stacking faults. The decrease in $J_c$ at a high EB dose is attributed to the extension of the amorphous region of a non-superconducting phase.