• 제목/요약/키워드: B-doping

검색결과 254건 처리시간 0.029초

Cu가 도핑된 LSM의 구조분석과 열팽창특성 연구 (Structural analysis and thermal expansion property of Cu doped LSM for SOFCs)

  • 노태민;류지승;김진성;정철원;이희수
    • 한국결정성장학회지
    • /
    • 제21권4호
    • /
    • pp.175-180
    • /
    • 2011
  • 이종 원자가를 가시는 Cu의 도핑이 LSM에 미치는 영향을 구조적인 분석과 열팽창계수를 통해서 고찰하였다. 고상반응을 이용하여 $La_{0.8}Sr_{0.2}Mn_{1-x}Cu_xO_3$($0{\leq}x{\leq}0.3$)음 제조하였으며, Cu의 도핑 함량에 따른 결정구조 및 열팽창계수를 확인하였다. Cu 함량이 증가함에 따라서 격자상수외 열팽창계수가 감소하는 경향을 나타냈지만, x = 0.3인 경우에는 증가 하였다. 이러한 격자상수와 열팽창계수의 변화는 Cu 이온의 B-site에서의 Mn 자리에 치환될 때 $0{\leq}x{\leq}0.2$의 범위에서는 $Cu^{3+}$의 존재로 인한 이온 반성의 감소에 의한 것으로 판단되었고, x=0.3인 경우에는 $Cu^{2+}$$Mn^{4+}$의 존재로 인한 산소 공공의 증가에 기인한 것이었다.

Structure and Magnetic Properties of Ho and Ni Co-doped BiFeO3 Ceramics

  • Hwang, J.S.;Yoo, Y.J.;Park, J.S.;Kang, J.H.;Lee, K.H.;Lee, B.W.;Kim, K.W.;Lee, Y.P.
    • 한국진공학회:학술대회논문집
    • /
    • 한국진공학회 2014년도 제46회 동계 정기학술대회 초록집
    • /
    • pp.183-183
    • /
    • 2014
  • Recently, multiferroic materials gain much attention due to their fascinating fundamental physical properties. These materials offer wide range of potential applications such as data storage, spintronic devices and sensors, where both electronic and magnetic polarizations can be coupled. Among single-phase multiferroic materials, $BiFeO_3$ is typical because of the room-temperature magnetoelectric coupling in view of long-range magnetic- and ferroelectric-ordering temperatures. However, $BiFeO_3$ is well known to have large leakage current and small spontaneous polarization due to the existence of oxygen vacancies and other defects. Furthermore the magnetic moment of pure $BiFeO_3$ is very weak owing to its antiferromagnetic nature. Recently, various attempts have been performed to improve the multiferroic properties of $BiFeO_3$ through the co-doping at the A and the B sites, by making use of the fact that the intrinsic polarization and magnetization are associated with the lone pair of $Bi^{3+}$ ions at the A sites and the partially-filled 3d orbitals of $Fe^{3+}$ ions at the B sites, respectively. In this study, $BiFeO_3$, $Bi_{0.9}Ho_{0.1}FeO_3$, $BiFe_{0.97}Ni_{0.03}O_3$ and $Bi_{0.9}Ho_{0.1}Fe_{0.97}Ni_{0.03}O_3$ bulk compounds were prepared by solid-state reaction and rapid sintering. High-purity $Bi_2O_3$, $Ho_2O_3$, $Fe_2O_3$ and $NiO_2$ powders with the stoichiometric proportions were mixed, and calcined at $500^{\circ}C$ for 24 h to produce the samples. The samples were immediately put into an oven, which was heated up to $800^{\circ}C$ and sintered in air for 1 h. The crystalline structure of samples was investigated at room temperature by using a Rigaku Miniflex powder diffractometer. The field-dependent and temperature-dependent magnetization measurements were performed with a vibrating-sample magnetometer and superconducting quantum-interference device.

  • PDF

Crystalline Growth Properties of Diamond Thin Film Prepared by MPCVD

  • Park Soo-Gil;Kim Gyu-Sik;Einaga Yasuaki;Fujishima Akira
    • 전기화학회지
    • /
    • 제3권4호
    • /
    • pp.200-203
    • /
    • 2000
  • Microwave plasma chemical vapor deposition을 이용하여 붕소가 도핑된 전도성 다이아몬드 박막을 제조하였다. 탄소원으로는 아세톤과 메탄올을 사용하였으며, 붕소원으로는 $B_2O_3$를 사용하고, 운반가스로는 수소를 사용하였다. 이때 붕소의 도핑농도는 약 $10^2ppm\;(B/C)$이였다. Si 기질 각 부분의 온도와 플라즈마에서의 거리를 다르게 하기 위해서 Si 기질을 배치함에 있어 약$10^{\circ}$를 기울여 다이아몬드 박막을 성장시켰다. 실험결과 모두 동일한 조건 이였으나 같은 Si 기질 위에 높이에 따른 온도구배가 형성되었으며, 그에 따라 다이아몬드의 결정 또한 각기 달랐다. 다이아몬드 박막에 나타난 결정형태의 분포는 약 $3\~4$부분으로 나뉘어 있었다 제조된 다이아몬드 박막의 특성을 확인하기 위해 Raman spectrum을 이용해 다이아몬드의 결정성을 확인하였고, 표면의 형태를 관찰하기 위해 현미경을 사용하였다. 입자의 크기는 각기 다른 Si기질의 높이에 의한 온도구배로 인하여, 기질의 높이에 따라 서서히 달라졌다. 다이아몬드 박막의 Raman spectrum측정결과 $1334cm^{-1}$에서 강한 peak가 발견되었으며, 이것은 결정성 다이아몬드의 일반적인 특성 이였다. Si 기질 중 낮은 곳에 위치한 부분의 Raman spectrum은 비다이아몬드의 peak인 $1550cm^{-1}$ 부근에서 넓게 peak가 상승된 것이 관찰되었다.

Ba(Zn1/3Ta2/3)O3 마이크로파 유전체에서 ZrO2와 NiO의 비화학양론적 첨가 (Nonstoichiometric Addition of ZrO2 and NiO to the Ba(Zn1/3Ta2/3)O3 Microwave Dielectrics)

  • 남경덕;강성우;김태희;심수만;최선희;김주선
    • 한국전기전자재료학회논문지
    • /
    • 제24권12호
    • /
    • pp.955-961
    • /
    • 2011
  • We investigated the physical properties of stoichiometric and non-stoichiometric oxide doped complex perovskite, $Ba(Zn_{1/3}Ta_{2/3})O_3$ ceramics and their impacts on the microwave dielectric performances using various characterization techniques such as X-ray diffraction, scanning electron microscopy, transmission electron microscopy, and network analyzer. According to the measurement of lattice constant changes, anomalous lattice volume contraction of $ZrO_2$ doped $Ba(Zn_{1/3}Ta_{2/3})O_3$ sample only showed the dielectric quality factor enhancements, which was due to the lattice volume contraction as well as the 1:2 B-site cation ordering. In addition, NiO doping was useful to the stabilization of temperature coefficient of resonance frequency.

고체산화물 연료전지용 Strontium Titanate 세라믹 접속자 소재의 소결 거동 및 전기적 특성 (Sintering Behavior and Electrical Properties of Strontium Titanate-Based Ceramic Interconnect Materials for Solid Oxide Fuel Cells)

  • 박범경;이종원;이승복;임탁형;박석주;송락현;신동열
    • 한국신재생에너지학회:학술대회논문집
    • /
    • 한국신재생에너지학회 2010년도 추계학술대회 초록집
    • /
    • pp.80.1-80.1
    • /
    • 2010
  • A strontium titanate ($SrTiO_3$)-based material with a perovskite structure is considered to be one of the promising alternatives to $LaCrO_3$-based materials since $SrTiO_3$ perovskite shows a high chemical stability under both oxidizing and reducing atmospheres at high temperatures. $SrTiO_3$ materials exhibit an n-type semiconducting behavior when it is donor-doped and/or exposed to a reducing atmosphere. In this work, $Sr_{1-x}La_xTi_{1-y}M_yO_3$ materials doped with $La^{3+}$ in A-sites and aliovalent transition metal ions ($M^{n+}$) in B-sites were synthesized by the modified Pechini method. The X-ray diffraction analysis indicated that the materials synthesized by the Pechini process exhibited a single curbic perovskite-type structure without any impurity phases, and are tolerant, to some extent, to cation doping. The sintering behaviors of $Sr_{1-x}La_xTi_{1-y}M_yO_3$ in $H_2/N_2$ and air were characterized by dilatometry and microstructural observations. The electrical conduction mechanism and the dopant effect are discussed based on the defect structures and the electrical conductivities measured at various oxygen partial pressures and temperatures.

  • PDF

Effect of Ni dopant on the multiferroicity of BiFeO3 ceramic

  • Hwang, J.S.;Yoo, Y.J.;Kang, J.H.;Lee, K.H.;Lee, B.W.;Park, S.Y.;Lee, Y.P.
    • 한국진공학회:학술대회논문집
    • /
    • 한국진공학회 2016년도 제50회 동계 정기학술대회 초록집
    • /
    • pp.139.1-139.1
    • /
    • 2016
  • Multiferroic materials are of great interest because of its potential applications in the design of devices combining magnetic, electronic and optical functionalities. Among various multiferroic materials, $BiFeO_3$(BFO) is known to be one of the intensively focused mainly due to the possibility of multiferroism at device working temperature (> $200^{\circ}C$). However, leakage current and weak polarization resulting from oxygen deficiency and crystalline defect should be resolved. Furthermore the magnetic ordering of pure BFO mainly prefers to have antiferromagnetic coupling. Up to now many attempts have been performed to improve the ferromagnetic and the ferroelectric properties of BFO by doping. In this work, we investigated the effects of Ni substitution on the multiferroism of bulk BFO. Four BFO samples (a pure BFO and three Ni-doped BFO's; $BiFe_{0.99}Ni_{0.01}O_3$, $BiFe_{0.98}Ni_{0.02}O_3$ and $BiFe_{0.97}Ni_{0.03}O_3$) were synthesized by the standard solid-state reaction and rapid sintering technique. The XRD results reveal that Ni atoms are substituted into Fe-sites and give rise to phase transition of cubic to rhombohedal. By using vibrating sample magnetometer and standard ferroelectric tester, the multiferroic properties at room temperature were characterized. We found that the magnetic moment of Ni-doped BFO turned out to be maximized for 3% of Ni dopant.

  • PDF

마이크로 공진 구조체 제작을 위한 다층 폴리실리콘의 스트레스 특성 (Stress characteristics of multilayer polysilicon for the fabrication of micro resonators)

  • 최창억;이창승;장원익;홍윤식;이종현;손병기
    • 센서학회지
    • /
    • 제8권1호
    • /
    • pp.53-62
    • /
    • 1999
  • MEMS(Microelectromechanical System) 기술분야에서 폭넓게 사용하고 있는 폴리실리콘 박막을 이용하여 폴리실리콘 미소 공진 구조체를 제작하였다. 폴리실리콘 증착은 저압기상화학증착 장비를 사용하여 대칭적 두께로 박막을 적층하였고 폴리실리콘의 응력과 응력구배를 최소화시키기 위한 적층, 도핑 방법 및 열처리에 따른 특성을 분석하였다. 이를 위하여 브리지 빔과 캔티레바 테스트 패턴을 제작하여 기계적 응력 특성을 측정하였으며, 아울러 공정 조건별 개별 시료에 대한 물성을 XRD, SIMS등으로 분석하였다. 공진 구조체는 대칭적 증착 구조를 가지며, 최종적으로 $6.5{\mu}m$의 두께로 적층되었다. 제작된 평면형 공진 구조체의 진동특성은 직류 15V, 교류 0.05V의 구동전압, 1000mtorr 압력에서 공진 진폭이 $5{\mu}m$ Q값이 1270임을 보였으며, 개발된 마이크로 폴리실리콘 공진체는 마이크로 자이로 및 가속도 센서에 응용될 수 있다.

  • PDF

An Analytical Model of the First Eigen Energy Level for MOSFETs Having Ultrathin Gate Oxides

  • Yadav, B. Pavan Kumar;Dutta, Aloke K.
    • JSTS:Journal of Semiconductor Technology and Science
    • /
    • 제10권3호
    • /
    • pp.203-212
    • /
    • 2010
  • In this paper, we present an analytical model for the first eigen energy level ($E_0$) of the carriers in the inversion layer in present generation MOSFETs, having ultrathin gate oxides and high substrate doping concentrations. Commonly used approaches to evaluate $E_0$ make either or both of the following two assumptions: one is that the barrier height at the oxide-semiconductor interface is infinite (with the consequence that the wave function at this interface is forced to zero), while the other is the triangular potential well approximation within the semiconductor (resulting in a constant electric field throughout the semiconductor, equal to the surface electric field). Obviously, both these assumptions are wrong, however, in order to correctly account for these two effects, one needs to solve Schrodinger and Poisson equations simultaneously, with the approach turning numerical and computationally intensive. In this work, we have derived a closed-form analytical expression for $E_0$, with due considerations for both the assumptions mentioned above. In order to account for the finite barrier height at the oxide-semiconductor interface, we have used the asymptotic approximations of the Airy function integrals to find the wave functions at the oxide and the semiconductor. Then, by applying the boundary condition at the oxide-semiconductor interface, we developed the model for $E_0$. With regard to the second assumption, we proposed the inclusion of a fitting parameter in the wellknown effective electric field model. The results matched very well with those obtained from Li's model. Another unique contribution of this work is to explicitly account for the finite oxide-semiconductor barrier height, which none of the reported works considered.

Fe2O3첨가에 따른 (Na,K,Li)(Nb,Sb,Ta)O3계 세라믹스의 압전 및 유전 특성 (Piezoelectric and Dielectric Properties of (Na,K,Li)(Nb,Sb,Ta)O3 Ceramics as a Function of Fe2O3 Addition)

  • 이광민;신상훈;류주현
    • 한국전기전자재료학회논문지
    • /
    • 제27권9호
    • /
    • pp.555-560
    • /
    • 2014
  • In this paper, in order to develop outstanding Pb-free composition ceramics, the $Fe_2O_3$-doped ($Na_{0.525}K_{0.443}Li_{0.037}$)($Nb_{0.883}Sb_{0.08}Ta_{0.037}$)$O_3$ + 0.3 wt% $Bi_2O_3$ + x wt% $Fe_2O_3$ (x= 0~1.0 wt%)(abbreviated as NKL-NST) lead-free piezoelectric ceramics have been synthesized using the ordinary solid state reaction method. The effect of $Fe_2O_3$-doping on their microstructure and electrical properties were investigated. XRD diffraction pattern studies confirm that $Fe_2O_3$ completely diffused into the NKL-NST lattice to form a new stable soild solution with $Fe^{3+}$ entering the $Nb^{5+}$, $Sb^{5+}$ and $Ta^{5+}$ of B-site. And, phase structure of all the ceramics exhibited pure perovskite phase and no secondary phase was found in the ceramics. The ceramics doped with 0.6 wt% $Fe_2O_3$ have the optimum values of piezoelectric constant($d_{33}$), planar piezoelectric coupling coefficient($k_p$) and mechanical quality factor($Q_m$) : $d_{33}$ = 233 [pC/N], $k_p$= 0.44, $Q_m$= 95. These results indicate that the ($Na_{0.525}K_{0.443}Li_{0.037}$)($Nb_{0.883}Sb_{0.08}Ta_{0.037}$)$O_3$ +0.3 wt% $Bi_2O_3$ + 0.6 wt% $Fe_2O_3$ ceramic is a promising candidate for lead-free piezoelectric ceramics.

Photoelectrochemical Cell Study on Closely Arranged Vertical Nanorod Bundles of CdSe and Zn doped CdSe Films

  • Soundararajan, D.;Yoon, J.K.;Kwon, J.S.;Kim, Y.I.;Kim, S.H.;Park, J.H.;Kim, Y.J.;Park, D.Y.;Kim, B.C.;Wallac, G.G.;Ko, J.M.
    • Bulletin of the Korean Chemical Society
    • /
    • 제31권8호
    • /
    • pp.2185-2189
    • /
    • 2010
  • Closely arranged CdSe and Zn doped CdSe vertical nanorod bundles were grown directly on FTO coated glass by using electrodeposition method. Structural analysis by XRD showed the hexagonal phase without any precipitates related to Zn. FE-SEM image showed end capped vertically aligned nanorods arranged closely. From the UV-vis transmittance spectra, band gap energy was found to vary between 1.94 and 1.98 eV due to the incorporation of Zn. Solar cell parameters were obtained by assembling photoelectrochemical cells using CdSe and CdSe:Zn photoanodes, Pt cathode and polysulfide (1M $Na_2S$ + 1M S + 1M NaOH) electrolyte. The efficiency was found to increase from 0.16 to 0.22 upon Zn doping. Electrochemical impedance spectra (EIS) indicate that the charge-transfer resistance on the FTO/CdSe/polysulfide interface was greater than on FTO/CdSe:Zn/polysulfide. Cyclic voltammetry results also indicate that the FTO/CdSe:Zn/polysulfide showed higher activity towards polysulfide redox reaction than that of FTO/CdSe/polysulfide.