• 제목/요약/키워드: Lattice Constant

검색결과 409건 처리시간 0.024초

Ln0.7Ca0.3MnO3 (Ln=Nd, Sm, La)의 소결 거동 및 특성 (Sintering behavior and characterization of Ln0.7Ca0.3MnO3 (Ln=Nd, Sm, La))

  • 전검배;구본흔;이찬규
    • 한국재료학회지
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    • 제16권1호
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    • pp.44-49
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    • 2006
  • Effects of doping rare earth element on Ln site of $Ln_{0.7}Ca_{0.3}MnO_3$ (Ln=Nd, Sm and La) were examined from sintering behavior, structure and magnetic properties. Sintering reactions proceeded rapidly in order of $La_{0.7}Ca_{0.3}MnO_3>Nd_{0.7}Ca_{0.3}MnO_3>Sm_{0.7}Ca_{0.3}MnO_3$. This result can be explained by diffusivity of metal cation. Size of a-axis increased as following order of La$Nd_{0.7}Ca_{0.3}MnO_3$, 93K for $Sm_{0.7}Ca_{0.3}MnO_3$ and 225K for $La_{0.7}Ca_{0.3}MnO_3$ were obtained. This result coincides with change of Mn-O bond length causing by a-axis lattice constant.

금속의 특성 및 금속수소화물의 팽창에 관한 수치해석 (Numerical Study on Properties of Metals and Expansion of Metal Hydrides)

  • 정영관;박규섭
    • 한국수소및신에너지학회논문집
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    • 제15권4호
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    • pp.257-265
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    • 2004
  • Numerical analysis, as EAM(Embedded Atom Method), in the atomic level is necessary to analyze the relation between the hydrogen and hydrogen absorption metals. EAM established on density functional theory was developed as a new means for calculating various properties and phenomena of realistic metal systems. In this study, we had constructed the EAM program from constitutive formulae and parameters of the hydrogen, nickel and palladium for the purpose of predicting the expansion behavior on hydrogen absorbing. In result, not only the ground state properties of metals but also lattice constants and the volume expansion ratio of metal hydrides show good agreement with Daw's data and experiment data.

수열합성 Ba-Ferrite분말의 조성과 자성에 미치는 열처리 효과 (Effects of Heat Treatment on the Composition and Magnetic Properties of the Hydrothermal-Synthesized Ba-Ferrite Powder)

  • 이승호;김중호;김태옥
    • 한국세라믹학회지
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    • 제26권6호
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    • pp.737-746
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    • 1989
  • After Ba-ferrite powders synthesized hydrothermally and its heated powders were dissolved partially with HCl treatment time, the BaO/Fe2O3 mole ratio of dissolved solutions and powders were measured by AAS, also, lattice constants, particle morphology and magnetic properties in HCl treated, heated and no-heated Ba-ferrite powders were abtained by means of XRD, SEM and VSM, respectively. From above analysis results, the effect of Ba/Fe mole ration in suspension(as starting material) on the BaO/Fe2O3 composition and particle characteristics of products were investigated, and the effect of heat treatment on magnetic properties of products examined. The composition, lattice constant and crystal phase of products depend on the Ba/Fe mole ratio in suspension. Ba content in surface or outer part of Ba-ferrite powder is higher than inner and heterogeneous, and the excess Ba ions in the inner part of particle move into the outer by heating, so that the mole ratio of BaO/Fe2O3 in the more jinner approaches more to the stoichiometric composition 1 : 6. The crystallinity, coercivity and saturation magnetization of products are increased by heat treatment, and the heat-treated samples synthesized hydrothermally in lower temperature are appreciated to have better powder characteristics.

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Investigation of Lattice Effects in Perovskites by $O-isotope^{18}$ Exchange

  • Itoh, Mitsuru;Mahesh, Rajappan;Wang, Ruiping
    • The Korean Journal of Ceramics
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    • 제6권3호
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    • pp.309-314
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    • 2000
  • In the present study, preliminary experimental results of the change in the properties of perovskite-type oxides caused by the $^{18}O$- exchange have been reported. Two systems were selected for the exchange, (1) $ATiO_3$(A=Ca,Sr,Ba) and (2) manganese perovskite. The dielectric properties of isotope-exchanged $SrTi^{18}O_3$showed a drastic change from a quantum paraelectricity below 3K to ferroelectric-like behavior with a peak at 23K and an enhanced dielectric constant, 35000 at the peak. On the contrary, the $T_c$ for $BaTiO_3$was found to increase by 0.9K. The observed isotope shift of $T_c$ as well as $T_co$ for the manganese perovskites is correlated with the key parameters controlling the lattice such as $Mn^{3+}$ content, average ionic radius of the A-site cation <$r_A$> ad A-site ionic disorder $\sigma^2$.

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PST (20/80)/ PST(80/20) 이종층 박막의 유전특성 (Dielectric properties of PST (20/80)/ PST(80/20) heterolayered thin films)

  • 김경태;김관하;우종창;김종규;강찬민;김창일
    • 대한전기학회:학술대회논문집
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    • 대한전기학회 2006년도 추계학술대회 논문집 전기물성,응용부문
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    • pp.115-116
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    • 2006
  • Dielectric PST (20/80) / PST (80/20) heterolayered thin films structures were created by a consequent deposition of the PST (20/80) and PST (80/20) thin films on the $Pt/Ti/SiO_2/Si$ substrate using alkoxide-based sol-gel method. Both structural and dielectric properties of heterolayered PST thin films were investigated for the tunable microwave device applications. As the number of coating increases, the lattice distortion decreased. It can be assumed that the lower PST layer affects a nucleation site or a seeding layer for the formation of the upper PST layer. The dielectric constant, dielectric loss and tunability of the PST-6 heterolayered structure measured at 100 kHz were 399, 0.022 and 57.9%, respectively. All these parameters showed an increase with increasing number of coatings due to the decrease in lattice distortion.

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아크센서를 적용한 격자형 용접용 모빌 로봇의 제어 (Motion Control of Mobile Robot with Arc Sensor for Lattice Type Welding)

  • 전양배;한영대;김상봉
    • 대한기계학회:학술대회논문집
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    • 대한기계학회 2001년도 춘계학술대회논문집B
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    • pp.319-324
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    • 2001
  • This paper presents the motion control of a mobile robot with arc sensor for lattice type welding. Its dynamic equation and motion control method for welding speed and seam tracking are described. The motion control is realized in the view of keeping constant welding speed and precise target line even though the robot is driven along a straight line or corner. The mobile robot is modeled based on Lagrange equation under nonholonomic constraints and the model is represented in state space form. The motion control of the mobile robot is separated into three driving motions of straight locomotion, turning locomotion and torch slider controls. For the torch slider control, the proportional integral derivative (PID) control method is used. For the straight locomotion, a concept of decoupling method between input and output is adopted and for the turning locomotion, the turning speed is controlled according to the angular velocity value at each point of the comer with range of $90^{\circ}$ constrained to the welding speed. The experiment has been done to verify the effectiveness of the proposed controllers. These results are shown to fit well by the simulation results.

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광 CT용 자성 가넷 막의 에피택시 육성 및 평가 (Epitaxial Growth and Evaluation of Magnetic Garnet Films for Optical Current Transducers)

  • 조재경
    • 한국자기학회지
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    • 제17권6호
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    • pp.246-252
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    • 2007
  • 본 논문에서는 출발원료 배합비 및 육성 파라미터가 LPE(Liquid Phase Epitaxy)법으로 육성된 자성 가넷 막의 특성에 미치는 영향을 조사하며, 광 CT의 페러데이 회전자용으로서 적합한 막의 육성 조건을 제시한다. 막을 평가하기 위하여 조사한 특성은 막후, 표면 모폴로지, X선 회절, 격자상수, 막과 기판(단결정 비자성 가넷 웨이퍼)사이의 격자상수의 부정합, 페러데이 회전각 등이었다. 또한, 육성된 자성 가넷 막을 이용하여 광 CT를 제작하고, 성능을 평가했다.

Ti-M-V 합금의 기지 및 제 2상의 수소화 특성 (Hydrogenation Characteristics of the Matrix and the Second Phases of Ti-M-V Alloys)

  • 조성욱
    • 한국수소및신에너지학회논문집
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    • 제14권2호
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    • pp.97-104
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    • 2003
  • The structural transitions of the matrix and the second phases of $Ti_{1.0}Mn_{0.9}V_{1.1}$ and $Ti_{1.0}Cr_{1.5}V_{1.7}$ alloys upon hydrogenation have been investigated at 293K. The effect of hydrogen isotope on their crystal structures has been also discussed. The crystal structures, Phase abundance and lattice parameters of the hydrides were determined by the Rietveld method using X-ray diffraction data. At the experimental temperature, the $Ti_{1.0}Mn_{0.9}V_{1.1}$ alloy and $Ti_{1.0}Cr_{1.5}V_{1.7}$ alloy revealed different structural transition processes upon hydrogenation although the crystal structures of these two alloys are both BCC at room temperature. The second phases such as Ti-rich phase with $NiTi_2$ structure and $\alpha$-Ti with HCP structure absorbed hydrogen at relatively low hydrogen pressures and the phase abundance remained almost constant. This means that it is desirable to decrease the amount of the second phases as far as possible in order to increase the effective hydrogen storage capacities of the alloys. The crystal structures of corresponding isotope hydrides, the phase abundance and the lattice parameters did not depend on the kind of hydrogen isotope, but only on the hydrogen content.

$Zn_{0.5}Cd_{0.5}Al_{2}Se_{4}$$Zn_{0.5}Cd_{0.5}Al_{2}Se_{4}:Co^{2+}$ 단결정의 광학적 특성과 열역학 함수 추정 (Optical properties and thermodynamic function properties of undoped and Co-doped $Zn_{0.5}Cd_{0.5}Al_{2}Se_{4}$ Single Crystals)

  • 현승철;김형곤;김덕태;박광호;박현;오석균
    • 대한전기학회:학술대회논문집
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    • 대한전기학회 2002년도 학술대회 논문집 전문대학교육위원
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    • pp.88-93
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    • 2002
  • $Zn_{0.5}Cd_{0.5}Al_{2}Se_{4}$ and $Zn_{0.5}Cd_{0.5}Al_{2}Se_{4}:Co^{2+}$ + single crystals were grown by CTR method. The grown single crystals have defect chalcopyrite structure with lattice constant a= 5.5966A. c= 10.8042${{\AA}}$ for the pure. a= 5.6543${{\AA}}$. c= 10.8205${{\AA}}$ for the Co-doped single crystal. respectively. The optical energy band gap was given as indirect band gap. The optical energy band gap was decreased according to add of Co-impurity. Temperature dependence of optical energy band gap was fitted well to the Varshni equation. From this relation. we can deduced the entropy. enthalpy and heat capacity. Also. we can observed the Co-impurity optical absorption peaks assigned to the $Co^{2+}$ ion sited at the $T_d$ symmetry lattice and we consider that they were attributed to the electron transitions between energy levels of ions.

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Structural nature of chemically inequivalent borons in the nonlinear optical material β-BaB2O4 studied using 11B MAS NMR and 11B single-crystal NMR

  • Kim, Woo Young;Lim, Ae Ran
    • 한국자기공명학회논문지
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    • 제17권2호
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    • pp.86-91
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    • 2013
  • Detailed information about the structural nature of three-coordinate borons in ${\beta}-BaB_2O_4$ is obtained through $^{11}B$ MAS NMR and $^{11}B$ single-crystal NMR. The three-coordinate $BO_3$ of the two borons B(1) and B(2) in ${\beta}-BaB_2O_4$ were distinguished. The spin-lattice relaxation time in the laboratory frame $T_1$ for B(1) and B(2) slowly decreases with increasing temperature, whereas the spin-lattice relaxation time in the rotating frame $T_{1{\rho}}$ for B(1) and B(2), which differs from $T_1$, is nearly constant. The B(1) and B(2) of the two types were distinguished by $^{11}B$ MAS NMR and $^{11}B$ single-crystal NMR.