• 제목/요약/키워드: Ferroelectric ceramics

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La 첨가량에 따른 $Bi_{4-x}La_{x}Ti_{3}O_{12}$ 강유전체의 주파수특성 (The Ferroelectric Frequency characteristics of $Bi_{4-x}La_{x}Ti_{3}O_{12}$ ceramics with the variation of Lanthanum additives)

  • 김응권;박복기;박기엽;박춘배
    • 한국전기전자재료학회:학술대회논문집
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    • 한국전기전자재료학회 2001년도 추계학술대회 논문집 Vol.14 No.1
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    • pp.463-466
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    • 2001
  • In recent year, Ferroelectric $BLT(Bi_{4-x}La_{x}Ti_{3}O_{12})$ is a promising candidate materials. This study was practiced to make good conditions of BL T targets. In this study, calcination and sintering temperature were kept at $750^{\circ}C$, $1100^{\circ}C$ for 2 hour respectively. the density obtained 7.612, 7.98, $7.877g/cm^{3}$ as $La_{2}O_{3}$ contents were 0.0mol%, 0.25mol%, 0.5mol%. Especially, the lanthanum content of 0.5 mol% measured C-axis (117) preferred orientation more than the others targets in the XRD. In $\varepsilon_{r}-f$ relationship using by HP 4194 A impedance analyzer, the 0.5 mol% observed above 200 relative dielectric constant. but the dissipation factor was higher than others targets at 100Hz~13MHz range. SEM photograph with the content of $La_{2}O_{3}$ was observed like rod and plate types.

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La 첨가량에 따른 Bi$_{4-x}La_x$Ti$_3O_12$ 강유전체의 주파수특성 (The Ferroelectric Frequency characteristics of Bi$_{4-x}La_x$Ti$_3O_12$ ceramics with the variation of Lanthanum additives)

  • 김응권;박복기;박기엽;박춘배
    • 한국전기전자재료학회:학술대회논문집
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    • 한국전기전자재료학회 2001년도 추계학술대회 논문집
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    • pp.463-466
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    • 2001
  • In recent year, Ferroelectric BLT($Bi_{4-x}$La$_{x}$Ti$_3$O$_{12}$) is a promising candidate materials. This study was Practiced to make good conditions of BLT targets. In this study, calcination and sintering temperature were kept at 75$0^{\circ}C$, 110$0^{\circ}C$ for 2 hour respectively. the density obtained 7.612, 7.98, 7.877 g/㎤ as La$_2$O$_3$ contents were 0.0mol%, 0.25mo1%, 0.5mol%. Especially, the lanthanum content of 0.5 mol% measured C-axis (117) preferred orientation more than the others targets in the XRD. In $\varepsilon$$_{r}$-f relationship using by HP 4194 A impedance analyzer, the 0.5 mol% observed above 200 relative dielectric constant. but the dissipation factor was higher than others targets at 100Hz~13MHz range. SEM photograph with the content of La$_2$O$_3$ was observed like rod and plate types.types.s.

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투광성 $Ba(La_{1/2}Nb_{1/2})O_3-PbZrO_3-PbTiO_3$ 세라믹의 강유전 및 전기광학 특성에 관한 연구 (A Study on the Ferroelectric and Electro-Optical Properties of the Transparent $Ba(La_{1/2}Nb_{1/2})O_3-PbZrO_3-PbTiO_3$ Ceramics)

  • 김준수;류기원;이성갑;이영희
    • 대한전기학회:학술대회논문집
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    • 대한전기학회 1991년도 추계학술대회 논문집 학회본부
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    • pp.325-328
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    • 1991
  • In this study, $0.085Ba(La_{1/2}Nb_{1/2})O_3-0.915Pb(Zr_yTi_{1-y})O_3$(y=0.45, 0.50, 0.55, 0.60, 0.65[mol]) transparent electrooptic ceramics were fabricated by two-stage sintering method. Increasing the $PbZrO_3$ contents, dielectric constant was increased and Curie temperature was decreased. In the composition of 0.55[mol] $PbZrO_3$, electromechanical coupling factor was 0.43. From the results of ferroelectric hysteresis loop and transmitted light intensity with electric field, the compositions of 0.65, 0.60, 0.55[mol] $PbZrO_3$ was applicable to electroopticmemory device and the compositions of 0.50, 0.45[mol] $PbZrO_3$ was applicable to linear electrooptic device.

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Powder Preparation by Hydroxide Coprecipitation and Phase Development of Pb0.97La0.02(Zr0.64Sn0.25Ti0.11)O3 Ceramics

  • Lee, Joon-Hyung;Chiang, Yet-Ming
    • The Korean Journal of Ceramics
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    • 제4권3호
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    • pp.260-267
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    • 1998
  • A homogeneous and stoichimetric fine powder of the ferroelectric $Pb_[0.97}La_{0.02}(Zr_{0.64}Sn_{0.25}Ti_{0.11})O_3$ (PLZST) has been prepared by the hydroxide coprecipitation method. Studies on the crystallization behavior of precursor as a function of temperature by X-ray powder diffraction and transmission electron microscopy technique were consistent with the formation of the pyrochlore phase from amorphous, initially at low temperatures around 500~$550^{\circ}C$. Further heat treatment up to $750^{\circ}C$ resulted in development of the perovskite phase with no significant pyrochlore crystallite growth. At intermediate temperatures the precursor yields a fine mixture of pyrochlore and perovskite phases. When the pyrochlore phase was heat teated in air, slight weight increase was observed in the temperature range of 300~$700^{\circ}C$, which is thought to be caused from oxygen absorption. In argon atmosphere, weight increase was not observed. On the other hand, weight loss began to occur near $700^{\circ}C$, with giving off mostly CO2 gas. This implies that the pyrochlore phase seems to be crystallorgraphycally and thermodynamically metastable. An apparent activation energy of 53.9 ㎉/mol was estimated for the pyrochlore-perovskite phase transformation.

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$BaTiO_3$의 강유전-상유전 상전이에 미치는 A($Cu_{1/3}Nb_{2/3}$)$O_3$ (A=Pb, Ba 및 Sr)의 영향 (Influences of A($Cu_{1/3}Nb_{2/3}$)$O_3$(A=Pb, Ba and Sr) on the Ferroelectric Paraelectric Phase Transition of $BaTiO_3$ Ceramics)

  • 박휴범;김정;김시중
    • 한국세라믹학회지
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    • 제28권12호
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    • pp.969-974
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    • 1991
  • The influences of A(Cu1/3Nb2/3)O3(A=Pb, Ba and Sr) on the ferroelectric-paraelectric phase transition of BaTiO3 ceramics has been investigated. The tetragonality of crystal structure decreased with increasing A(Cu1/3Nb2/3)O3 content at room temperature. A linear correlation between Curie point and the tetragonality of lattice was not observed. In all three systems the variation of Curie point with the mole fraction showed similar tendency that the Curie point decreased at lower mole fraction but gradually increased in the region of higher mole fractions, Diffuse phase transitions were observed at higher mole fractions. The variation of Curie points could be explained by internal stress and Jahn-Teller distortion of BO6 due to Cu2+, and it was thought that the diffuse character of phase transition was caused by compositional fluctuation.

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Pb($Zn_{1/3}Nb_{2/3})O_3-Pb(Zr_xTi{1-x})O_3$세라믹의 구조적, 전기적 특성 (Structure and Electrical Properties of Pb($Zn_{1/3}Nb_{2/3})O_3-Pb(Zr_xTi{1-x})O_3$ Ceramics)

  • 조현무;이성갑;이영희
    • 한국전기전자재료학회:학술대회논문집
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    • 한국전기전자재료학회 2000년도 하계학술대회 논문집
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    • pp.357-360
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    • 2000
  • Ferroelectric 0.05PZN-xPZT(90/10)-(0.95-x)PZT(10/90) (x=0.65, 0.85) specimens were fabricated by the mixed-oxide method and cold-pressing method using sol-gel derived PZT(90/10) and PZT(10/90) powders. All specimens show a uniform ferroelectric grain without the presence of the pyrocholre phase. Average grain size increased with an increase in sintering temperature, the value for the x=0.65 specimen sintered at 125$0^{\circ}C$ was 14.4${\mu}{\textrm}{m}$. The dielectric constant and dielectric loss of the x=0.65 specimen sintered at 125$0^{\circ}C$ were 1247, 2.05%, respectively. All specimens showed fairly good temperature and frequency stability of dielectric constant with the range from -2$0^{\circ}C$ to 6$0^{\circ}C$ and 100Hz to 10MHz. The coercive electric field and the remanent polarization of x = 0.65 specimen sintered at 125$0^{\circ}C$ were 8.5 kV/cm and 13 $\mu$C/cm$^2$, respectively.

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Preparation and Characterization of Small Sized PZT Powders: A Sol-Gel Modified Approach

  • 최규만;이해춘
    • 한국정보전자통신기술학회논문지
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    • 제1권2호
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    • pp.27-32
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    • 2008
  • A current research basically diverted towards an increase in the operational output with the minimization of the materials used, which ultimately scaled down the dimensions of ceramic electronic components. In this direction the nano-technology pave the revolutionary changes in particular the electronic industries. The applications of nano-sized particles or nano-sized materials are hence, playing a significant role for various purposes. The PZT(lead, zirconium, titanium) based ceramics which, are reported to be ferroelectric materials have their important applications in the areas of surface acoustic waves (SAW), filters, infrared detectors, actuators, ferroelectric random access memory, speakers, electronic switches etc. Moreover, these PZT materials possess the large electro mechanical coupling factor, large spontaneous polarization, low dielectric loss and low internal stress etc. Hence, keeping in view the unique properties of PZT piezoelectric ceramics we also tried to synthesize indigenously the small sized PZT ceramic powder in the laboratory by using the modified sol-gel approach. In this paper, propyl alcohol based sol-gel method was used for preparation of PZT piezoelectric ceramic. The powder obtained by this sol-gel process was calcined and sintering to reach a pyrochlore-free crystal phase. The characterization of synthesized material was carried out by the XRD analysis and the surface morphology was determined by high resolution scanning electron microscopy.

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Effect of RTA Treatment on $LiNbO_3$ MFS Memory Capacitors

  • Park, Seok-Won;Park, Yu-Shin;Lim, Dong-Gun;Moon, Sang-Il;Kim, Sung-Hoon;Jang, Bum-Sik;Junsin Yi
    • The Korean Journal of Ceramics
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    • 제6권2호
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    • pp.138-142
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    • 2000
  • Thin film $LiNbO_3$MFS (metal-ferroelectric-semiconductor) capacitor showed improved characteristics such as low interface trap density, low interaction with Si substrate, and large remanent polarization. This paper reports ferroelectric $LiNbO_3$thin films grown directly on p-type Si (100) substrates by 13.56 MHz RF magnetron sputtering system for FRAM (ferroelectric random access memory) applications. RTA (rapid thermal anneal) treatment was performed for as-deposited films in an oxygen atmosphere at $600^{\circ}C$ for 60sec. We learned from X-ray diffraction that the RTA treated films were changed from amorphous to poly-crystalline $LiNbO_3$which exhibited (012), (015), (022), and (023) plane. Low temperature film growth and post RTA treatments improved the leakage current of $LiNbO_3$films while keeping other properties almost as same as high substrate temperature grown samples. The leakage current density of $LiNbO_3$films decreased from $10^{-5}$ to $10^{-7}$A/$\textrm{cm}^2$ after RTA treatment. Breakdown electric field of the films exhibited higher than 500 kV/cm. C-V curves showed the clockwise hysteresis which represents ferroelectric switching characteristics. Calculated dielectric constant of thin film $LiNbO_3$illustrated as high as 27.9. From ferroelectric measurement, the remanent polarization and coercive field were achieved as 1.37 $\muC/\textrm{cm}^2$ and 170 kV/cm, respectively.

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