• 제목/요약/키워드: Relaxor ferroelectrics

검색결과 35건 처리시간 0.039초

$Pb(Fe _{1/2}Ta_{1/2})O_3$의 합성, 유전특성 및 질서배열구조 (Syntheses, Dielectric Properties and Ordering Structures of $Pb(Fe _{1/2}Ta_{1/2})O_3$)

  • 우병철;김병국;김병호
    • 한국결정학회지
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    • 제13권3_4호
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    • pp.165-171
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    • 2002
  • 고상반응법에 의해 합성된 분말을 $1100^{\circ}C$에서 소결함으로써 밀도가 $9.3g/cm^3$이고 평균입경이 $5.1{\pm}1.2{\mu}$$Pb(Fe_{1/2}Ta_{1/2})O_3$를 단일상으로 합성하였다. (공간군: Pm3m) $-150{\sim}50^{\circ}C$에서 측정된 비유전율은 인가전압의 주파수가 1kHz일 때 $-41^{\circ}C$에서 비유전율이 3100으로 최대값을 가지고 유전완화(dielectric relaxation)현상 및 완만한 상전이(diffuse phase transition, DPT)가 뚜렷하게 관찰되는 전형적인 완화형 강유전특성을 보였으며 소결후 $1000^{\circ}C$에서의 열처리 시간이 증가함 에 따라 상전이의 완만화도는 감소하여 정상 강유전체화 하였다. 한편, 소결직후 $Fe^{3+}$$Ta^{5+}$ 이온은 투과전자현미경으로도 검출할 수 없는 정도의 단거리 영역에서 화학양론적으로 1 : 1 질서 배열하고 있으며 이러한 B자리 양이온의 질서배열은 열처리 시간이 증가함에 따라 강화됨을 라만분광법으로 확인하였다. 소결직후 $Pb(Fe^{12}Ta_{1/2})O_3$센서의 완화형 강유전특성은 B자리 양이온의 화학양론적 1:1 단거리 질서배열구조와, 열처리한 $Pb(Fe_{1/2}TA_{1/2})O_3$에서의 완화형 강유전특성 감소는 열처리에 따라 강화된 화학양론적 1:1 단거리 질서배열구조와 연관지을 수 있었다.

Effect of Nb Doping on the Dielectric and Strain Properties of Lead-free 0.94(Bi1/2Na1/2)TiO3-0.06BaTiO3 Ceramics

  • Han, Hyoung-Su;Hong, In-Ki;Kong, Young-Min;Lee, Jae-Shin;Jo, Wook
    • 한국세라믹학회지
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    • 제53권2호
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    • pp.145-149
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    • 2016
  • $(Bi_{1/2}Na_{1/2})_{0.94}Ba_{0.06}(Ti_{1-x}Nb_x)O_3$ (BNBTxNb) ceramics were investigated in terms of the crystal structure as well as the ferroelectric, dielectric, and piezoelectric properties. While little change was observed in the microstructure except for a slight decrease in the average grain size, a significant change was noticed in the temperature dependence of dielectric and piezoelectric properties. It was shown that the property changes are closely related to the downward shift in the position of the ferroelectric-to-relaxor transition temperature with increasing amount of Nb doping. A special emphasis is put on the fact that Nb doping is so effective at decreasing the ferroelectric-to-relaxor transition temperature that even at no more than 2 at.% Nb addition, the transition temperature was already brought down slightly below room temperature, resulting in the birth of a large strain at 0.46 %, equivalent to $S_{max}/E_{max}=767pm/V$.

Pb계 Perovskite-Pyrochlore 복합체의 강유전특성 (Ferroelectric Characteristics of Pb-containing Perovskite-Pyrochlore Composites)

  • 조진우;손정호;조상희
    • 한국세라믹학회지
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    • 제34권5호
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    • pp.500-504
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    • 1997
  • Perovskite Pb0.7Ba0.3Zn1/3Nb2/3O3 substituted with 0.3 mole fraction for Pb-site in PbZn1/3Nb2/3O3 relaxor and pyrochlore Pb1.83Ba0.29Zn1.71Nb2/3O6.39 were mixed and dielectric characteristics of this composites were investigated. Percolation limit of perovskite phase, which was determined by microstructural observation in the composite as an isolation of perovskite phase from pyrochlore matrix, was 28.9-47.5 vol%. Ferroelectric phase transition below percolation limit depends on a parameter which affects the propagation of lattice vibration between isolated perovskite phase and pyrochlore matrix. Therefore, it is believed that ferroelectric lattice vibration of isolated perovskite phase could be transfered to pyrochlore matrix when the oxygen octahedra are linked in 3-dimension and highly polarizable Pb2+ ions are contained in both phases.

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Dielectric and Electrical Properties of Ce,Mn:SBN

  • Kang, Bong-Hoon;Paek, Young-Sop;Rhee, Bum-Ku;Lim, Ki-Soo;Joo, Gi-Tae
    • 한국세라믹학회지
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    • 제40권7호
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    • pp.615-619
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    • 2003
  • Temperature and frequency dependence of dielectric and electrical properties was investigated in cerium and manganese doped Sr$\_$0.6/Ba$\_$0.4/Nb$_2$O$\_$6/(60SBN) ceramic system. Structural deformation of 60SBN by dopants did not appeared. 1350$^{\circ}C$-10 h sintered specimen had higher densification than 1250$^{\circ}C$-10 h sintered one, to which dielectric properties are related. That the feature of dielectric maxima peaks was typical Diffusive Phase Transition (DPT), it was explained by "random-field Ising model". Even though 60SBN has large dielectric loss at high frequency above 100 ㎑, it is desirable for optical applications because of low dielectric loss at low frequency. From Arrhenius plot of temperature, the activation energy was calculated to 0.45-0.49 eV.

$Pb(Mg_{1/3}Nb_{2/3})O_3-PbZrO_3$계 요업체의 전계 유기변위와 분극특성 (Field-induced Strains and Polarization Switching Mechanisms in $Pb(Mg_{1/3}Nb_{2/3})O_3-PbZrO_3$ Ceramics)

  • 김명철
    • 한국세라믹학회지
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    • 제34권6호
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    • pp.569-576
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    • 1997
  • Electrically-induced strain and polarization studies of the (1-x)Pb(Mg1/3Nb2/3)O3-PbZrO3 crystalline solutions have been done. Dielectric constants with temperature were investigated for 0$\leq$x$\leq$0.95. With increasing PbZrO3 content the transition maxima were found to move to higher temperature region and DPT (Diffused Phase Transition) properties were decreased for x$\leq$0.60. Phase transition between ferroelectric states and antiferroelectric states was confirmed for 0.93$\times$10-3 for 0.4

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완화형 강유전체 PMN-PT계에서 약전계 및 강정계 조건에서의 relaxation 거동 (Dielectric Relaxation in PMN-PT Relaxor Ferroelectrics under Weak and Strong Electric Field)

  • 박재환;김윤호;박순자
    • 한국재료학회지
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    • 제8권2호
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    • pp.95-98
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    • 1998
  • 완화형 강유전체인 0.9MPb*Mg$_{1}$3/Nb$_{2}$3/)O$_{3}$-0.1PbTiO$_{3}$에서 강유전-상유전 상전이에 수반되는 relaxation거동을 살펴보기위해 낮은 전계에서 측정된 유전특성과 높은 전계에서 측정된 전계유기 분극 거동 등을 조사하였다. -50-9$0^{\circ}C$의 상전이 온도범위에 걸쳐 1V/mm의 낮은 전계에서 측정된 유전특성의 온도의존성을 구하고 수 kVmm의 강전계하에서 발생된 분극의 온도의존성을 관찰하였다. 이 모든 결과들은 Vogel-Fulcher관계식에 비교적 정확하게 일치되었으며 그 결과 T$_{f}$ 는 294.6˚K로 나타났다. 본 연구결과를 통하여 Vogel-Fulcher관계식에 의한 주파수 의존성은 낮은 전계하에서의 유전특성 뿐 아니라 강전계하에서의 여러물성들도 동일하게 적용되는 것을 확인할 수 있었다.

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PMN계 완화형 강유전체에서 전왜특성의 온도 의존성 (Temperature Dependence of the Electric-field-induced Strains in PMN-based Relaxor Ferroelectrics)

  • 박재환;홍국선;박순자
    • 한국재료학회지
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    • 제6권4호
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    • pp.349-356
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    • 1996
  • 완화형 강유전체의 가장 대표적인 PMN계에서 첨가제의 종류와 함량, 측정온도, 인가 전계의형태 등의 변화에 따른 전계인가 변화특성을 광법위하게 조사하였다. Columbite precursor법에의해 분말을 준비하고 고상소결방법에 의하여 모든 시편을 제조하였다. 순수한 PMN에 첨가제로서 PbTiO3와 Pb(Zr, Ti)O3를 첨가한 경우에 완전한 perovskite 구조의 고용체가 형성되었음을 알 수 있었다. T$\varepsilon$max이상에서는 변위의 이력이 크게 발생하는 강유전체의 거동을 보여주었다. 양방향으로 전계를 인가하여 변위를 이용하면 발생 strain은 실온 근방에서 온도에 대하여 안정적이지만 단방향 전계에 따른 변위는 온도에 따라 크기가 변한다는 것을 알 수 있었고 유전상수가 큰 경우가 전왜의 크기 또한 큰 것을 알 수 있었다. 0.9MN-0.1PT와 0.8PMN-0.2PZT의 경우 최대가 되는 온도는 유전율이 최대가 되는 온도보다 더 낮은 온도에서 나타났다.

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Stabilization of the Perovskite Phase and Electrical Properties of Ferroelectrics in the Pb2(Sc,Nb)O6 System

  • Kim, Yeon Jung
    • Applied Science and Convergence Technology
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    • 제24권6호
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    • pp.224-227
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    • 2015
  • Ferroelectric $Pb_2(Sc,Nb)O_6$ were prepared under two different sintering conditions using the oxide mixing method and the electrical properties were measured. The sintering conditions were $1350^{\circ}C$ for 25 minutes and $1400^{\circ}C$ for 20 minutes. EDX spectroscopy and XRD were used to determine the crystalline characteristic of the $Pb_2(Sc,Nb)O_6$ compositions Pyrochlore phase showed about 2% in all $Pb_2(Sc,Nb)O_6$ specimens. It expands the growth of crystals in samples sintered at $1400^{\circ}C$ than $1350^{\circ}C$, but all samples were the optimal crystallization. The temperature and frequency dependence of the complex dielectric constant and admittance were measured to analyze the electrical properties. The high dielectric constant of the specimens reflects the good stoichiometry and crystallization. The maximum value of the dielectric constant in the two specimens treated with sintering at $1350^{\circ}C$ and $1400^{\circ}C$ were more than 27,000, and the dielectric loss at room temperature is smaller than 0.05. The maximum dielectric constant decreased with increasing frequency, the transition temperature also increased in $Pb_2(Sc,Nb)O_6$ compositions. The admittance and susceptance values reach a peak at all temperatures, and the magnitude of the peak increases with increasing measuring temperature. Strong frequency dependent of maximum admittance, susceptance, dielectric constant and dielectric loss were observed.

Scanning Force Microscope에 의한 (001) PMN-x%PT 단결정의 도메인 구조에 대한 연구 (Investigation of Domain Structure in (001) PMN-x%PT Crystals by Scanning Force Microscope)

  • 이은구;이재갑
    • 한국재료학회지
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    • 제19권6호
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    • pp.300-304
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    • 2009
  • The domain structures of annealed (001)-oriented $Pb(Mg_{1/3}Nb_{2/3})O_3-x%PbTiO_3$ (PMN-x%PT) crystals for x = 10, 20, 30, 35, and 40 at% were investigated by Polarized Optical Microscopy (POM) and Scanning Force Microscopy (SFM) in the piezoresponse mode. Both Polar Nano-Domains (PND) and long strip-like domains were clearly observed. The results also showed how the domain structure changed between phases with an increasing x in the PMN-x%PT crystals and the domain hierarchy on various length scales ranging from 40 nm to 0.1 mm. Distorted pseudo-cubic phase (x < 20%) consisted of PNDs that did not self-assemble into macro-domain plates. The rhombohedral phase (x = 30%) consisted of PNDs that began to self-assemble into colonies along preferred {110} planes. The monoclinic phase (x = 35%) consisted of miniature polar domains on the nm scale, whereas, the tetragonal phase (x = 40%) consisted of {001} oriented lamella domains on the mm scale that had internal nano-scale heterogeneities, which self-assembled into macro-domain plates oriented along {001} the mm scale.

Effect of Internal Bias Field on Poling Behavior in Mn-Doped Pb(Mg1/3Nb2/3)O3-29 mol%PbTiO3 Single Crystal

  • Lee, Geon-Ju;Kim, Hwang-Pill;Lee, Ho-Yong;Jo, Wook
    • 한국전기전자재료학회논문지
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    • 제34권5호
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    • pp.382-385
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    • 2021
  • Electrical poling is a crucial step to convert ferroelectrics to piezoelectrics. Nevertheless, no systematic investigation on the effect of poling has been reported. Given that the poling involves an alignment of spontaneous polarization, the condition for poling should be different when a material has an internal bias field that influences the domain stability. Here, we present the effect of poling profile on the dielectric and piezoelectric properties in Mn-doped Pb(Mg1/3Nb2/3)O3-29 mol%PbTiO3 single crystal with an internal bias field. We showed that both the dielectric permittivity and the piezoelectric coefficient were further enhanced when the poling procedure ends with a field application along the opposite direction to the internal bias field. We expect that the current finding would give a clue to understanding the true mechanism for the electrical poling.