• Title/Summary/Keyword: Lead zirconate titanate

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Co-firing of PZT/metal foil laminates for MIM structured device fabrication

  • Kim, Baek-Hyeon;Bae, Hyeon-Jeong;Gwon, Do-Gyun
    • Proceedings of the Materials Research Society of Korea Conference
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    • 2012.05a
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    • pp.82.2-82.2
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    • 2012
  • 캐패시터, 액추에이터와 같이 MIM (Metal-Insulator-Metal) 구조를 갖는 디바이스는 높은 소결온도를 갖는 세라믹 유전체/압전체와 고온 내산화성이 낮은 금속 전극의 적층 형태로 인하여 동시 열처리 공정에 있어서 많은 제약이 따른다. 본 연구에서는 소결온도를 대폭 낮춘 저온 소결용 PZT 압전체 테이프를 니켈 금속 포일에 적층하여 동시 열처리를 통하여 소결을 시도하였다. 동시 열처리된 MIM 디바이스의 세라믹과 금속 전극 계면의 미세구조 및 성분 분석을 통하여 계면 반응 기구를 확인하였고, 계면 반응층이 디바이스의 특성에 미치는 영향에 대한 정량적 분석을 수행하였다. 또한 열처리 시간에 따른 계면 반응층의 변화를 관찰하고 반응층의 변화가 특성에 미치는 영향을 분석하였다. 니켈 이외에 니켈 합금인 INCONEL 718과 PZT 세라믹과의 동시 소성을 시도하여 니켈, INCONEL 두 금속 기판과 PZT 사이에 생성되는 계면 반응층의 미세구조와 특성의 차이점을 비교하였고 디바이스로서 사용하기 위한 적합성 여부를 확인하였다.

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Stress Development in Sol-gel Derived Multideposited Coatings of Lead Zirconate Titanate (다층 도포된 $\textrm{PbZr}_{0.53}\textrm{Ti}_{0.47}\textrm{O}_{3}$ sol-gel 박막내의 응력 거동)

  • Park, Sang-Myeon
    • Korean Journal of Materials Research
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    • v.9 no.11
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    • pp.1069-1074
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    • 1999
  • 본 연구에서는 PbZr(sub)0.53Ti(sub)0.47O$_3$(PZT) 박막을 복수 도포함에 따른 박막내의 응력을 온도의 함수로 실시간(in situ) 측정하였으며, 응력발생의 원인에 박막의 건조, 열분해(pyrolysis), 치밀화 및 결정화 현상과 연관시켜 설명하였다. 도포직후 단층박막에 생성된 55MPa의 인장응력은 가열됨에 따라$ 300^{\circ}C$-$350^{\circ}C$에서 최대 145MPa로 증가하였으며, 박막내의 응력은 모든 온도구간에서 항상 인장응력을 나타내었더. 다층도포시 $650^{\circ}C$까지 열처리 주기를 완료한 층이 두꺼워질수록 새로 도포한 층의 영향은 점차 감소하였으며, 9층박막에 이르러서는 가열과 냉각에 따라 응력이 동일하게 변화하였다. 응력측정 결과 다층박막의 치밀화는 $350^{\circ}C$에서 시작되어 $520^{\circ}C$-$550^{\circ}C$ 부근에서 완료되는 것으로 나타났으며 치밀화가 시작하는 온도는 미세경도 측정결과와 일치하였다. $PbTiO_3$(PT)와 달리 PZT 다층박막은 Si 기판 위에서 perovskite로의 결정화가 일어나지 않았다.

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The Seeding Effects on the Phase Transformation of Sol-Gel Derived PZT Powder

  • Lee, Hyun-Tae;Lee, Wan-In;Kim, Yoo-Hang;Whang, Chin-Myung
    • Bulletin of the Korean Chemical Society
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    • v.23 no.8
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    • pp.1078-1084
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    • 2002
  • The formation temperature for the perovskite lead zirconate titanate [Pb(Zr,Ti)O3, PZT] derived from sol-gel route was lowered by more than $100^{\circ}C$ with the addition of crystallographically suitable seed particles, such as barium titanat e (BT) or PZT. We investigated the effect of seeding on the crystallization of perovskite phase and in the microstructure of the sol-gel derived PZT powder by varying the concentration, size and chemical species of seed particles. The phase transition as a function of temperature was monitored by DTA, XRD, and Raman spectroscopy, and the interface between the seed particle and grown PZT layer was analyzed by SEM and high resolution TEM techniques. It was found that both the heterogeneous and homogeneous nucleation contributes competitively in the formation of perovskite PZT grains.

Sol-Gel Processing and Properties of PZT Powders and Thin Films (졸-겔법에 의한 PZT 합성과 박막제조)

  • 오영제;정형진
    • Journal of the Korean Ceramic Society
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    • v.28 no.12
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    • pp.943-952
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    • 1991
  • Lead zirconate titanate(PZT) powders and thin films were prepared from an alkoxide-based solution by sol-gel method. Gelation of synthesized complex solutions, pyrolysis and crystallization behaviors of the dried powder were studied in accordance with a water content and a catalyst. PZT thin films were formed by spin-casting method on silicon and platinum substrates, and characterized. Ester produced from the reactions was completely removed when drying of the gel was finished. Pyrolysis property of the dried PZT gels were changed in order water content, class of catalyst, and quantity of catalyst. Crystalline Pb phase was transiently formed near 250$^{\circ}C$. Basic catalyst is good additive for a formation of perovskite phase in the films, and acidic catalyst for a densified film structure. By the analysis of RBS, Pb element in the PZT films were diffused into silicon substrate, and the pores, may be produced due to local densification around some grains in the films, make an origin of fault in microstructure when holding time goes to be longer at 700$^{\circ}C$.

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Construction and Application of Experimental Formula for Nonlinear Behavior of Ferroelectric Ceramics Switched by Electric Field at Room Temperature during Temperature Rise

  • Ji, Dae Won;Kim, Sang-Joo
    • Journal of the Korean Ceramic Society
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    • v.55 no.1
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    • pp.67-73
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    • 2018
  • A poled lead zirconate titanate (PZT) cube specimen that is switched by an electric field at room temperature is subject to temperature increase. Changes in polarization and thermal expansion coefficients are measured during temperature rise. The measured data are analyzed to obtain changes in pyroelectric coefficient and strain during temperature change. Empirical formulae are developed using linear or quadratic curve fitting to the data. The nonlinear behavior of the materials during temperature increase is predicted using the developed formulae. It is shown that the calculation results can be compared successfully with the measured values, which proves the accuracy and reliability of the developed formulae for the nonlinear behavior of the materials during temperature changes.

An anisotropic ultrasonic transducer for Lamb wave applications

  • Zhou, Wensong;Li, Hui;Yuan, Fuh-Gwo
    • Smart Structures and Systems
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    • v.17 no.6
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    • pp.1055-1065
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    • 2016
  • An anisotropic ultrasonic transducer is proposed for Lamb wave applications, such as passive damage or impact localization based on ultrasonic guided wave theory. This transducer is made from a PMNPT single crystal, and has different piezoelectric coefficients $d_{31}$ and $d_{32}$, which are the same for the conventional piezoelectric materials, such as Lead zirconate titanate (PZT). Different piezoelectric coefficients result in directionality of guided wave generated by this transducer, in other words, it is an anisotropic ultrasonic transducer. And thus, it has different sensitivity in comparison with conventional ultrasonic transducer. The anisotropic one can provide more information related to the direction when it is used as sensors. This paper first shows its detailed properties, including analytical formulae and finite elements simulations. Then, its application is described.

Compensation of temperature effect on impedance responses of PZT interface for prestress-loss monitoring in PSC girders

  • Huynh, Thanh-Canh;Kim, Jeong-Tae
    • Smart Structures and Systems
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    • v.17 no.6
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    • pp.881-901
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    • 2016
  • In this study, a method to compensate the effect of temperature variation on impedance responses which are used for prestress-loss monitoring in prestressed concrete (PSC) girders is presented. Firstly, an impedance-based technique using a mountable lead-zirconate-titanate (PZT) interface is presented for prestress-loss monitoring in the local tendon-anchorage member. Secondly, a cross-correlation-based algorithm to compensate the effect of temperature variation in the impedance signatures is outlined. Thirdly, lab-scale experiments are performed on a PSC girder instrumented with a mountable PZT interface at the tendon-anchorage. A series of temperature variation and prestress-loss events are simulated for the lab-scale PSC girder. Finally, the feasibility of the proposed method is experimentally verified for prestress-loss monitoring in the PSC girder under temperature-varying conditions and prestress-loss events.

Fabrication of PZT Tubular Structures by a Template-wetting Process

  • Shaislamov, U.A.;Hong, S.K.;Yang, B.
    • Journal of the Korean Ceramic Society
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    • v.44 no.5 s.300
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    • pp.141-143
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    • 2007
  • Nanotubes and microtubes of ferroelectric lead zirconate titanate (PZT) were synthesized by means of a simple and convenient process called a template-wetting process. Nanoporous alumina and macroporous Si were used as template materials to fabricate the corresponding tubes. For the improvement of the wetting properties of the wetting solution, the PZT solution was mixed with a polymer. The polymer was removed completely during annealing. The grain growth processes of the PZT nanotubes during baking and furnace annealing were examined by means of field emission electron microscope (FE-SEM) and X-ray diffractometry (XRD).

Measured Polarization Hysteresis and Predicted Reference Remnant Polarization and Strains of Ferroelectric Ceramics at Various Electric Field Loading Rates and Temperatures (다양한 전계인가율과 온도에서 강유전 세라믹의 이력선도 계측과 기준 잔류 분극 및 변형률 거동 예측)

  • Ji, Dae Won;Kim, Sang-Joo
    • Journal of the Korean Ceramic Society
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    • v.51 no.6
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    • pp.591-597
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    • 2014
  • A poled lead zirconate titanate (PZT) rectangular parallelepiped specimen was subjected to through-thickness electric fields at five loading rates and four temperatures. The rates of the electric field were 0.01, 0.10, 0.25, 0.50, and $1.00MVm^{-1}s^{-1}$; the temperatures were 20, 50, 80, and $110^{\circ}C$. From the measured polarization hysteresis responses, the so-called reference remnant polarization and strains were calculated. Using the calculated reference remnant polarization hysteresis loops, the effects of loading rates and temperature were discussed; using the calculated reference remnant strains, strain butterfly loops were calculated and compared with observations.

Experiment and Prediction of Nonlinear Behavior at High Temperatures of Ferroelectric Ceramics Switched by Electric Field at Room Temperature

  • Ji, Dae Won;Kim, Sang-Joo
    • Journal of the Korean Ceramic Society
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    • v.54 no.3
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    • pp.235-242
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    • 2017
  • Changes in polarization and thermal expansion coefficients during temperature increase of a poled lead zirconate titanate (PZT) cube specimen switched by an electric field at room temperature are measured. The measured data are analyzed to construct governing differential equations for polarization and strain changes. By solving the differential equations, an experimental formula for the high temperature behavior of ferroelectric materials is obtained. It is found that the predictions by the formula are in good agreement with measures. From the viewpoint of macroscopic remnant state variables, it appears that the processes of electric field-induced switching at different temperatures are identical and independent of temperature between $20^{\circ}C$ and $110^{\circ}C$.