• 제목/요약/키워드: Ferroelectric phase

검색결과 365건 처리시간 0.024초

<001> 0.7Pb(Mg1/3Nb2/3)O3-0.3PbTiO3 단결정의 상변화 및 유전 특성 (Phase Transformation and Dielectric Properties of <001> 0.7Pb(Mg1/3Nb2/3)O3-0.3PbTiO3 Single Crystals)

  • 이은구;이재갑
    • 한국재료학회지
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    • 제21권7호
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    • pp.391-395
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    • 2011
  • The structure and dielectric properties of poled <001>-oriented 0.7Pb($Mg_{1/3}Nb_{2/3})O_3-0.3PbTiO_3$ (PMN-0.3PT) crystals have been investigated for orientations both parallel and perpendicular to the [001] poling direction. An electric field induced monoclinic phase was observed for the initial poled sample. The phase remained stable after the field was removed. A quite different temperature dependence of dielectric constant has been observed between heating and cooling due to an irreversible phase transformation. The results of mesh scans and temperature dependence of the dielectric constant demonstrate that the initial monoclinic phase changes to a single domain tetragonal phase at 370K and to a paraelectric cubic phase at 405K upon heating. However, upon subsequent cooling from the unpoled state, the cubic phase changes to a poly domain tetragonal phase and to a rhombohedral phase. In the ferroelectric tetragonal phase with a single domain state, the dielectric constant measured perpendicular to the poling direction was dramatically higher than that of the parallel direction. A large dielectric constant implies easier polarization rotation away from the polar axis. This enhancement is believed to be related to dielectric softening close to the morphotropic phase boundary and at the phase transition temperature.

$BaTiO_3$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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졸-겔법으로 형성한 강유전체 PZT박막의 고온 단시간 열처리효과 및 전자 디바이스에의 응용 (The rapid thermal annealing effects and its application to electron devices of Sol-Gel derived ferroelectric PZT thin films)

  • 김광호
    • E2M - 전기 전자와 첨단 소재
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    • 제7권2호
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    • pp.152-156
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    • 1994
  • The rapid thermal annealing effects of Sol-Gel derived ferroelectric PZT thin films were investigated. It was found that rapid thermal annealing(RTA) of spin coated thin films on silicon typically >$800^{\circ}C$ for about 1 min. was changed to the perovskite phase. Rapid thermally annealed films recorded maximum remanent polarization of about 5 .mu.C/cm$^{2}$, coercive field of around 30kV/cm. The switching time for polarization reversal was about 220ns. The films of RTA process showed smooth surface, and high breakdown voltages of over 1 MV/cm and resistivity of $1{\times}{10^12}$ .ohm.cm at 1 MV/cm. It was verified that the polarization reversal of the PZT film was varied partially with applying the multiple short pulse.

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PZT 박막 캐패시터의 2차 고조파 전류특성 (The Second Harmonic Current Characteristic of PZT Thin Film Capacitor)

  • 김동철;박봉태;고중혁;문병무
    • 한국전기전자재료학회논문지
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    • 제11권8호
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    • pp.596-600
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    • 1998
  • A method for the nondestructive read-out of the memory in ferroelectric thin films is demonstrated using the detection second harmonic currents introduced in the ferrolelectric capacitor as a response to an ac signal. The sign and phase of the second harmonic current depends on the polarized state +$P_r or -P_r$, The studied ferroelectric PZT thin film is found to have desirable features for the use as a memory element. This method and material seems as a promising approach for the nonvolatile memory storage.

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Ferroelectric Properties of Seeded SBT Thin Films on the LZO/Si Structure

  • Im, Jong-Hyun;Jeon, Ho-Seung;Kim, Joo-Nam;Lee, Gwang-Geun;Park, Byung-Eun;Kim, Chul-Ju
    • 한국전기전자재료학회:학술대회논문집
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    • 한국전기전자재료학회 2007년도 추계학술대회 논문집
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    • pp.128-129
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    • 2007
  • We fabricated seeded $SrBi_2Ta_2O_9$(SBT) thin films using seeding technique on the $LaZrO_x$ (LZO)/Si structure. To evaluate the ferroelectric properties of seeded SBT thin films, we investigated the crystalline phase, the surface morphology, the capacitance-voltage (C-V) curve and the current density-voltage (J-V) curve of seeded films and then compared with the physical and electrical properties of unseeded films. As the result of that, the characteristics of seeded and unseeded films have a slight difference. Therefore, the ferroelectric properties of seeded SBT thin films are not necessarily superior than unseeded films.

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Effect of Poling Electric Field and Temperature Change on the Dielectric Anomalies of Relaxor Ferroelectric Strontium-Barium-Niobate Single Crystals

  • Shabbir, Ghulam;Ko, Jae-Hyeon;Kojima, Seiji
    • Journal of the Korean Physical Society
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    • 제73권10호
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    • pp.1561-1565
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    • 2018
  • The dielectric properties of the uniaxial relaxor ferroelectric $Sr_xBa_{1-x}Nb_2O_6$ with x = 0.75 were investigated along the polar [001] direction as a function of temperature. The capacitance maximum showed the frequency dispersion commonly observed in relaxors. Additional weak dielectric anomalies were observed in the paraelectric phase; they were only seen during the heating process and disappeared upon subsequent cooling. These were attributed to the existence of large polar clusters strongly pinned at defects and/or to random fields and their metastable characters. Aligning the ferroelectric domains along the polar axis at room temperature removed the high-temperature dielectric anomalies. The dependences of the capacitance and the dielectric maximum temperature on the magnitude of the poling field were investigated.

Heterostructure 열처리에 의한 Bi 조성 제어가 SrBi$_2$Ta$_{2-x}$Nb$_x$O$_9$ 박막의 강유전 특성에 미치는 영향 (The Effect of Bismuth Composition Controlled by Heat Treating Heterostructure on the Ferroelectric Properties of SrBi$_2$Ta$_{2-x}$Nb$_x$O$_9$ Thin Films)

  • 박윤백;이전국;정형진;박종완
    • 한국세라믹학회지
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    • 제35권10호
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    • pp.1040-1048
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    • 1998
  • Ferroelectric properties of{{{{ { { { {SrBi }_{2 }Ta }_{2-x }Nb }_{x }O }_{9 } }} (SBIN) thin films were affected by the amount of Bi content in SBTN. The addition of Bi into the SBTN films could be accomplished by heat treating SBTN/Bi2O3/SBTN het-erostructures fabricated by r.f. magnetron sputtering method. The variation of Bi content was controlled by changing the thickness of the sandwiched Bi2O3 in SBTN/Bi2O3/SBTN heterostructure from 50 to 400$\AA$. As changing the thickness of the sandwiched Bi2O3 in Bi2O3 films was increased from 0 to 100$\AA$ the grain grew faster and the ferroelectric pro-perties were improved. On the other hand when the thickness of Bi2O3 films was thicker than 150$\AA$ the fer-roelectric properties were deteriorated Especially for SBTN thin films inserted by 400$\AA$ Bi2O3 layer a Bi2Phase appeared as a second phase resulting in poor ferroelectric properties. The maximum remanent po-larization (2Pr) and coercive field(Ec) were obtained for the SBTN/Bi2O3/(100$\AA$)/SBTN thin films. In this case 2Pr and Ec were 14.75 $\mu$C/cm2 and 53.4kV/cm at an applied voltage of 3V respectively.

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중심그룹으로 Bipheny1 ester기를 갖는 새로운 강유전성 액정 (Nes ferroelectric liquid crystal having bipeny1 ester core group)

  • 전영재;이종천;김용배
    • 한국재료학회지
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    • 제4권6호
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    • pp.695-703
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    • 1994
  • 4-(4-Alkyloxybenzoyloxy)-4'-(S)-$\alpha$-halo-alkanoyloxybipeny1계열 액정화합물이 합성되고, 그들의 액정성질이 조사되었다. 합성된 바이페닐 에스터계열 화합물들은 키랄 스메틱 C상 뿐 아니라 키랄 네마틱 및 스메틱 A상을 나타내고, $10^{-7}\textrm{cm}^2$ 이상의 큰 자발분극을 나타내었다.

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VDF/TrFE 공중합체(共重合體)의 강유전특성(强誘電特性) (A Study on Ferroelectric Properties of VDF/TrFE copolymer)

  • 방태찬;강대하
    • 대한전기학회:학술대회논문집
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    • 대한전기학회 1996년도 하계학술대회 논문집 C
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    • pp.1472-1475
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    • 1996
  • D-E hysteresis loops have been measured for the 65/35 mole % copolymer of vinylidene fluoride and trifIuoroethyIene over wide temperature range. The results were analyzed and discussed. The remanent polarization and the coercive field at room termperature were estimated to be 75 $mC/m^3$ and 55 MV/m respectively. D-E hysteresis loops were observed even below the glass transiation temperature$-20^{\circ}C$) and the remanent polarization and the coercive field were larger than larger, as the temperature lower. It seems that the remanent polarization and the coercive field depend on the amorphous region as well as crystalline region in this copolymer. And the ferroelectric-to-paraelectric phase transition was observed at $90^{\circ}C$ on heating and $80^{\circ}C$ on cooling. Double hysteresis loops were observed at the temperature($85^{\circ}C$) of paraelectric phase.

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2단 소성시간이 7.6/70/30 PLZT 세라믹의 전기적 특성에 미치는 영향 (Electro-optic Characteristics of 7.5/70/30 PLZT Ceramics According to the Second Stage Sintering Time)

  • 박창엽;정익채;정희승
    • 대한전기학회:학술대회논문집
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    • 대한전기학회 1987년도 정기총회 및 창립40주년기념 학술대회 학회본부
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    • pp.220-223
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    • 1987
  • In this paper, electro-optic characteristics of PLZT 7.6/70/30 composition in MPB regions, which antiferroelectric and ferroelectric phases coexist together, were studied. As sintering times are increased, Curie temperatures ore linearly decreased. And the antiferroelectric phase becomes more stronger when Curie temperatures are decreased. The crystal structure investigated by lie of X-ray analysis is proved to cubic in the thermally depoled specimen and rhombohedral in the poled specimen. Accordingly, the applicability of 7.6/70/30 specimen as image storage and display device is expected by the method for applying field induced reversible transitions between antiferroelectric(AFE) and ferroelectric(FE) phase.

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