• 제목/요약/키워드: ferroelectricity

검색결과 75건 처리시간 0.019초

BaTiO3 첨가에 따른 Bi1/2Na1/2TiO3-SrTiO3 무연 압전 세라믹스의 전기적 특성 및 상전이 거동 연구 (Electrical Properties and Phase Transition Behavior of Lead-Free BaTiO3-Modified Bi1/2Na1/2TiO3-SrTiO3 Piezoelectric Ceramics)

  • 강유빈;박재영;무클리사 아이샤 데비타;즈엉 짱 안;안창원;김병우;한형수;이재신
    • 한국전기전자재료학회논문지
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    • 제35권5호
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    • pp.516-521
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    • 2022
  • We investigated the microstructure, crystal structure, dielectric, and elecromechanical strain properties of lead-free BaTiO3 (BT)-modified (Bi1/2Na1/2)TiO3-SrTiO3 (BNT-ST) piezoelectric ceramics. Samples were prepared by a conventional ceramic processing route. Temperature dependent dielectric properties confirmed that a phase transition from a nonergodic relaxor to an ergodic relaxor was induced when the BT concentration reached 1.5 mol%, interestingly, where the average grain size reached a maximum value of 4.5 ㎛. At the same time, enhanced electromechanical strain (Smax/Emax = 600 pm/V) was obtained. It is suggested that the induced ferroelectric-relaxor phase transition by the BT modification is responsible for the enhancement of electromechanical strain in 1.5 mol% BT-modified BNT-ST ceramics.

Pyroelectricity of BaTiO3-doped PMNT ferroelectric system for pyroelectric sensor

  • Yeon Jung Kim
    • 한국표면공학회지
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    • 제56권6호
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    • pp.380-385
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    • 2023
  • In this study, an MPB PMNT system containing 0.05 to 0.10 wt.% BaTiO3 was synthesized using a traditional chemical method and its pyroelectricity was investigated. Pyroelectricity, dielectricity, and ferroelectricity of the synthesized BaTiO3-PMNT system were analyzed by heat treatment at 1240~1280 ℃ for 4 hours to evaluate its applicability as a pyroelectric sensor. Unlike the simple ABO3 ferroelectric, the BaTiO3-doped PMNT system exhibited phase transition characteristics over a wide temperature range typical of complex perovskite structures. Although no dramatic change could be confirmed depending on the amount of BaTiO3 added, stable pyroelectricity was maintained near room temperature and over a wide temperature range. When the amount of BaTiO3 added increased from 0.05BaTiO3-PMNT to 0.10BaTiO3-PMNT, the electric field slightly increased from 5.00×103 kV/m to 6.75×103 kV/m, and the maximum value of remanent polarization slightly increased from 0.223 C/m2 to 0.234 C/m2. The pyroelectric coefficients of 0.05BaTiO3-PMNT and 0.10BaTiO3- PMNT at room temperature were measured to be ~0.0084 C/m2K and ~0.0043 C/m2K, respectively. The relaxor ferroelectric properties of the BaTiO3-PMNT system were confirmed by analyzing the plot of Kmax/K versus (T-Tmax)γ. The BaTiO3-doped MPB PMNT system showed a distinct pyroelectric performance index at room temperature, and the values were Fv ~ 0.0362 m2/C, Fd ~ 0.575×10-4 Pa-1/2.

RF 마그네트론 스퍼터링법에 의해 증착된 SrBi$_2$$Nb_2$>$O_9$ 박막의 전기적 특성에 관한 연구 (Electrical Properties of SrBi$_2$$Nb_2$>$O_9$ Thin Films deposited by RF Magnetron Sputtering Method)

  • 조금석;최훈상;이관;최인훈
    • 한국재료학회지
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    • 제11권4호
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    • pp.290-293
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    • 2001
  • 세라믹 타겟인 Sr$_2$Nb$_2$O$_{7}$ (SNO)과 Bi$_2$O$_3$을 장착한 RF-마그네트론 스퍼터링을 이용하여 SrBi$_2$Nb$_2$O$_{9}$ (SBN) 박막을 p-type Si(100) 기판 위에 증착하였다. 증착시 두 타겟의 파워비를 조절하여 조성의 변화에 따른 SBN 박막의 구조적 및 전기적 특성을 조사하였다. 증착된 SBN 박막은 $700^{\circ}C$의 산소분위기에서 1시간 동안 열처리를 하였으며 상부전극으로 Pt를 증착한 후 산소분위기에서 30분 동안 $700^{\circ}C$에서 전극 후열처리를 실시하였다. 증착된 SBN 박막은 $700^{\circ}C$ 열터리 후에 페로브스카이트 상을 나타냈으며 SNO 타겟과 Bi$_2$O$_3$타겟의 파워가 120 W/100 W 일 때 가장 좋은 전기적 특성을 나타내었다. 이때의 조성은 EPMA(Electron Probe X-ray Micro Analyzer) 분석을 통하여 확인하였으며 Sr:Bi:Nb의 비가 약 1:3:2임을 나타내었다. 이러한 과잉의 Bi조성을 가진 SBN 박막은 3-9 V의 인가전압에서 1.8 V-6.3 V의 우수한 메모리 윈도우 값을 나타내었으며 누설전류 값은 인가전압 5 V에서 1.54$\times$$10^{-7}$ A/$\textrm{cm}^2$였다.

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전기열량소자용 Ag 첨가량에 따른 K(Ta,Nb)O3 세라믹스의 구조적·전기적 특성 (Structural and Electrical Properties of K(Ta,Nb)O3 Ceramics with Variation of Ag Contents for Electrocaloric Devices)

  • 이민성;박병준;임정은;이삼행;이명규;박주석;이성갑
    • 한국전기전자재료학회논문지
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    • 제34권6호
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    • pp.442-448
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    • 2021
  • In this work, the (K1-xAgx)(Ta0.8Nb0.2)O3 (x=0.1-0.4) ceramics were fabricated using mixed-oxide method, and their structural and electrical properties were measured. All specimens represented a pseudo cubic structure with the lattice constant of 0.3989 nm. When 0.4 mol of Ag was added, second phases induced from metallic Ag and K2(Ta,Nb)6O16 phase were observed. Dielectric constant and dielectric loss of K(Ta0.8Nb0.2)O3 specimen doped with 0.3 mol of Ag were 2,737 and 0.446, respectively. The curie temperature was about -5℃, which does not change with Ag addition. The remanent polarization began to decrease sharply around 12~15℃, and the temperature at which the remanent polarization began to decrease as the applied voltage increased shifted to the high temperature side. The electrocaloric effect (ΔT) and electrocaloric efficiency (ΔT/ΔE) of the (K0.7Ag0.3)(Ta0.8Nb0.2)O3 ceramics were 0.01024℃ and 0.01825 KmV-1, respectively.

반대칭 교환 상호작용을 갖도록 Fe-Site가 제어된 PbFe1/2Nb1/2O3의 강유전/자기적 특성 연구 (Investigation on Ferroelectric and Magnetic Properties of Pb(Fe1/2Nb1/2)O3 Fe-Site Engineered with Antisymmetric Exchange Interaction)

  • 박지훈;이주현;조재현;장종문;조욱
    • 한국전기전자재료학회논문지
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    • 제35권3호
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    • pp.297-302
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    • 2022
  • We investigated the origin of magnetic behaviors induced by an asymmetric spin exchange interaction in Fe-site engineered lead iron niobate [Pb(Fe1/2Nb1/2)O3, PFN], which exhibits a room-temperature multiferroicity. The magnitude of spin exchange interaction was regulated by the introduced transition metals with a distinct Bohr magneton, i.e., Cr, Co, and Ni. All compositions were found to have a single-phase perovskite structure keeping their ferroelectric order except for Cr introduction. We discovered that the incorporation of each transition metal imposes a distinct magnetic behavior on the lead iron niobate system; antiferro-, hard ferro-, and soft ferromagnetism for Cr, Co, and Ni, respectively. This indicates that orbital occupancy and interatomic distance play key roles in the determination of magnetic behavior rather than the magnitude of the individual Bohr magneton. Further investigations are planned, such as X-ray absorption spectroscopy, to clarify the origin of magnetic properties in this system.