• Title/Summary/Keyword: remanent polarization.

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Electrical Characteristics of PZT Thin film Deposited by Rf-magnetron Sputtering as Pb Excess Content of Target (Rf-sputtering법으로 증착한 PZT박막의 타겟의 Pb 함량에 따른 전기적 특성에 관한 연구)

  • Lee, Kyu-Il;Kang, Hyun-Il;Park, Young;Park, Ki-Yub;Song, Joon-Tae
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.16 no.3
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    • pp.186-189
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    • 2003
  • The role of excess Pb about the crystallization behavior and electrical properties in b(Zr$\sub$0.52/Ti$\sub$0.48/)O3(PZT) thin films has not been precisely defined. In this work, the effect of excess Pb content on the ferroelectric properties of these films was investigated. To analyze the effect, PZT films containing various amounts of excess Pb were Prepared. PZT thin films were deposited on the Pt/Ti bottom electrode by rf magnetron sputtering method and then they were crystallized by rapid thermal annealing (RTA). The experiment showed that all PZT films indicated perovskite polycrystalline structure with preferred orientation (111) and no pyrochlore phase was observed. As higher excess Pb was included, the films showed that value of leakage current shift from 2.03${\times}$10$\^$-6/ to 6.63 ${\times}$ 10$\^$-8/A/cm$^2$ at 100kV/cm, and value of remanent polarization shift from 8.587 ${\mu}$C /cm$^2$ to 4.256 ${\mu}$C/ cm$^2$. Electrical properties of PZT thin film affected by Pb excess content of target were explained to be caused of defect among space charges and defect grain boundaries.

Dielectric and Piezoelectric Properties of xPb(Al0.5Nb0.5)O3-(1-x)Pb(Zr0.52Ti0.48)O3 Thin films Prepared by PLD (PLD법으로 제작된 xPb(Al0.5Nb0.5)O3-(1-x)Pb(Zr0.52Ti0.48)O3박막의 유전 및 압전 특성)

  • 김민철;박용욱;최지원;강종윤;안병국;김현재;윤석진
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.16 no.9
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    • pp.795-800
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    • 2003
  • The dielectric and piezoelectric properties of the xPb(A $l_{0.5}$N $b_{0.5}$) $O_3$-(1-x)Pb(Z $r_{0.52}$ $Ti_{0.48}$) $O_3$ [xPAN-(1-x)PZT] thin films by pulsed laser deposition (PLD) were investigated as a function of PAN contents. The effect of texture on dielectric and piezoelectric properties of the 0.05PAN-0.95PZT thin films having the highest piezoelectric constant( $d_{33}$) was studied more precisely. For 0$\leq$x$\leq$0.15 compositions in xPAN-(1-x)PZT thin films, the well-developed perovskite phase with (111) preferred orientation was obtained at the deposition temperature of 50$0^{\circ}C$. With increasing PAN content, remanent polarization and coercive field decreased. The dielectric constant increased with an increase of PAN content until it reached 1450 at $\chi$= 0.05, and then decreased for higher PAN content. The maximum points of dielectric constant coincides with the maximum points of the piezoelectric constant $d_{33}$.33/.33/././.

Electrical Properties of Sol-gel Derived Ferroelectric Bi3.35Sm0.65Ti3O12 Thin Films by Rapid Thermal Annealing

  • Cho, Tae-Jin;Kang, Dong-Kyun;Kim, Byong-Ho
    • Transactions on Electrical and Electronic Materials
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    • v.6 no.2
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    • pp.51-56
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    • 2005
  • Ferroelectric Bi$_{3.35}$Sm$_{0.65}$Ti$_{3}$O$_{12}$(BSmT) thin films were synthesized using a sol-gel process. Bi(TMHD)$_{3}$, Sm$_{5}$(O$^{i}$Pr)13, Ti(O$^{i}$Pr)4 were used as the precursors, which were dissolved in 2­methoxyethanol. The BSmT thin films were deposited on Pt/TiO$_{x}$/SiO$_{2}$/Si substrates by spin­coating. The electrical properties of the thin films were enhanced using rapid thermal annealing process (RTA) at 600 $^{circ}$C for 1 min in O$_{2}$. Thereafter, the thin films were annealed from 600 to 720 $^{circ}$C in oxygen ambient for 1 hr, which was followed by post-annealed for 1 hr after depositing a Pt electrode to enhance the electrical properties. X-ray diffraction (XRD) and scanning electron microscopy (SEM) were used to analyze the crystallinity and surface morphology of layered perovskite phase, respectively. The remanent polarization value of the BSmT thin films annealed at 720 $^{circ}$C after the RTA treatment was 35.31 $\mu$C/cmz at an applied voltage of 5 V.

Low Temperature Sintering Process of Sol-gel Derived Ferroelectric Sr0.9Bi2.1Ta1.8Nb0.2O9 Thin films (Sol-gel 법으로 제조된 강유전체 Sr0.9Bi2.1Ta1.8Nb0.2O9 박막의 저온결정화 공정)

  • 김영준;김병호
    • Journal of the Korean Ceramic Society
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    • v.40 no.3
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    • pp.279-285
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    • 2003
  • Ferroelectric S $r_{0.9}$B $i_{2.1}$T $a_{1.8}$N $b_{0.2}$ thin films with 200 nm thicknesses were deposited on Pt/Ti $O_2$/ $SiO_2$/Si Substrates by a sol-gel method. In these experiments, Sr(O $C_2$ $H_{5}$)$_2$, Bi(TMHD)$_3$, Ta(O $C_2$ $H_{5}$)$_{5}$ and Nb(O $C_2$ $H_{5}$)$_{5}$ were used as precursors, which were dissolved in 2-methoxyethanol. After UV-irradiation and RTA processes, the remanent polarization value (2 $P_{r}$) of SBTN thin films with annealed at $650^{\circ}C$ was 8.49 and 11.94 $\mu$C/$\textrm{cm}^2$ at 3 V and 5 V, respectively.

Structure and Pyroelectrical Properties of Pb($Zn_{1/3}Nb_{2/3}$)$O_3$-Pb($Zr_{x}Ti_{1-x}$)$O_3$Compound Ceramics (Pb($Zn_{1/3}Nb_{2/3}$)$O_3$-Pb($Zr_{x}Ti_{1-x}$)$O_3$ 세라믹의 구조적, 초전 특성)

  • 조현무;이성갑;이영희
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2000.11a
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    • pp.543-546
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    • 2000
  • Ferroeleclric 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$\mu$m. The dielectric constant and dielectric loss of the x=0.65 specimen sintered at 125$0^{\circ}C$ were 1247, 2.06%, 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 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. The pyroelectric coefficient of the x=0.65 specimen sintered at 125$0^{\circ}C$ was 5.64$\times$10$^{-8}$ C/cm$^2$K, respectively.

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Piezoelectric properties and microstructure of 0.01Pb(Mg1/2W1/2)O3-0.41Pb(Ni1/3Nb2/3)O3-0.35PbTiO3-0.23PbZrO3thick film with particle size distribution (입자 크기 분포에 따른 0.01Pb(Mg1/2W1/2)O3-0.41Pb(Ni1/3Nb2/3)O3-0.35PbTiO3-0.23PbZrO3 후막의 미세구조 및 압전특성)

  • Moon, Hi-Gyu;Song, Hyun-Cheol;Kim, Sang-Jong;Choi, Ji-Won;Kang, Chong-Yun;Yoon, Seok-Jin
    • Journal of Sensor Science and Technology
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    • v.17 no.6
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    • pp.418-424
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    • 2008
  • The PZT based piezoelectric thick films prepared by screen printing method have been mainly used as a functional material for MEMS applications due to their compatibility of MEMS process. However the screen printed thick films generally reveal poor electrical and mechanical properties because of their porous microstructure. To improve microstructure we mixed attrition milled powder with ball milled powder of 0.01Pb$(Mg_{1/2}W_{1/2})O_3$-0.41Pb$(Ni_{1/3}Nb_{2/3})O_3$-$0.35PbTiO_3$-$0.23PbZrO_3$+0.1 wt% ${Y_2}{O_3}$+1.5 wt% ZnO composition. By mixing 25 % of attrition milled powder and 75 % of ball milled powder, the broadest particle size distribution was obtained, leading to a dense thick film with crack-free microstructure and improved dielectric properties. The X-ray diffraction analysis revealed that the film was in wellcrystallized perovskite phase. The remanent polarization was increased from $13.7{\mu}C/cm^2$ to $23.3{\mu}C/cm^2$ at the addition of 25 % attrition milled powder.

Dielectric and Piezoelectric Properties of 0.125PMN-0.435PT-0.44PZ Ceramics for Ultrasonic footer Applications (초음파 전동기용 0.125PMN-0.435PT-0.44PZ 세라믹스의 유전 및 압전특성)

  • Kim, Jin-Soo
    • Journal of Sensor Science and Technology
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    • v.6 no.5
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    • pp.392-399
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    • 1997
  • In this study, the effect of the sintering temperature on the dielectric and piezoelectric properties of 0.5 wt% $MnO_{2}$-doped $0.125Pb(Mg_{1/2}Nb_{2/3})O_{3}-0.435PbTiO_{3}-0.44PbZrO_{3}$ ceramics were investigated aiming at ultrasonic motor applications. From experimental result, it was found that the optimal sintering temperature condition was at $1270^{\circ}C$. The sample sintered at $1270^{\circ}C$ had density of $7.72\;g/cm^{3}$, dielectric constant of 570, dielectric loss of 0.82%, remanent polarization of $19.18{\mu}C/cm^{2}$, coercive field of 9.63 kV/cm, electromechanical coupling factor of radial mode of 55.1%, mechanical quality factor of 886. Temperature and frequency dependence of dielectric constant and dielectric loss of the sintered sample at $1270^{\circ}C$ was also investigated.

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Electrocaloric Effect in Heterolayered K(Ta,Nb)O3/Pb(Zr,Ti)O3 Thin Films Fabricated by Spin-Coating Method (스핀-코팅법으로 제작한 K(Ta,Nb)O3/Pb(Zr,Ti)O3 이종층 박막의 전기 열량 효과)

  • Yang, Young-Min;Yuk, Ji-Soo;Kim, Ji-Won;Yi, Sam-Haeng;Park, Joo-Seok;Kim, Young-Gon;Lee, Sung-Gap
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.33 no.6
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    • pp.465-470
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    • 2020
  • Heterolayered K(Ta,Nb)O3/Pb(Zr,Ti)O3 thin films on Pt/Ti/SiO2/Si substrates were prepared by a sol-gel process and spin-coating method. The structural and electrical properties were measured to investigate the possibility of application as an electrocaloric effect device. All specimens exhibited dense and uniform cross-sectional structures without pores, and the average thickness of the specimen coated six times was approximately 394 nm. Curie temperatures were observed at 5℃ or less in type-I and 10℃ in type-II specimens, respectively. Type-II specimens coated 6 times showed a relative dielectric constant of 758 and remanent polarization of 9.71 μC/㎠ at room temperature. The maximum electrocaloric effect occurred between 20 and 25℃, slightly higher than their Curie temperature, and the electrocaloric property (ΔT) of the type-II specimens coated 6 times was approximately 1.2℃ at room temperature.

Electrical properties of sol-gel derived $ PbZrO_3$-$PbTiO_3$-$Pb(Ni_{1/3}Nb_{2/3})O_3$ thin film (Sol-Gel 법에 의한$ PbZrO_3$-$PbTiO_3$-$Pb(Ni_{1/3}Nb_{2/3})O_3$)

  • 임무열;구경완;한상옥
    • Electrical & Electronic Materials
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    • v.10 no.2
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    • pp.134-140
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    • 1997
  • PbTiO$_{3}$-PbZrO$_{3}$-Pb(Ni$_{1}$3/Nb $_{2}$3/O$_{3}$)(PZT-PNN) thin films were prepared from corresponding metal organics partially stabilized with diethanolamine by the sol-gel spin coating method. Each mol rates of PT:PZ:PNN solutions were #1(50:40:10), #2(50:30:20), #3(45:35:20) and #4(40:40:20), respectively. The spin-coated PZT-PNN films were sintered at the temperature from 500.deg. C to 600.deg. C for crystallization. The P-E hysteresis curve was drawn by Sawyer-Tower circuit with PZT-PNN film. The coercive field and the remanent polarization of #4(40:40:20 mol%) PZT-PNN film were 28.8 kV/cm and 18.3 .mu.C/cm$^{2}$, respectively. Their dielectric constants were shown between 128 and 1120, and became maximum value in MPB(40:40:20 mol%). The leakage currents of PZT-PNN films were about 9.4x 10$^{-8}$ A/cm$^{2}$, and the breakdown voltages were about 0.14 and 1.1 MV/cm. The Curie point of #3(45:35:20 mol%, sintered at 600.deg. C) film was 330.deg. C.

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Electrical Properties of Integrated Ir/$IrO_2$/PZT/Pt/$IrO_2$/Ir Ferroelectric Capacitor on TiN/W Plug Structure (TiN/W 플러그 구조 위에 제작된 Ir/$IrO_2$/PZT/Pt/$IrO_2$/Ir 강유전체 커패시터의 전기적 특성)

  • Choi, J.H.;Kweon, S.Y.;Hwang, S.Y.;Kim, Y.J.;Son, Y.J.;Cho, S.S.;Lee, A.K.;Park, S.H.;Lee, B.H.;Park, N.K.;Park, H.C.;Chang, H.Y.;Hong, S.K.;Hong, S.J.
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2006.06a
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    • pp.321-322
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    • 2006
  • The electrical properties of PZT thin film capacitor on TiN/W plug structure were investigated for high density ferroelectric memory devices. In order to enhance the ferroelectric properties of PZT capacitor, the process conditions of bottom electrodes were optimized. The fabricated PZT capacitor on TiN/W plug showed good remanent polarization, leakage current, and contact resistance of TiN/W plug, which were $33\;{\mu}C/cm^2$, $1.2{\times}10^{-6}\;A/cm^2$, and 5.3 ohm/contact, respectively.

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