• Journal of Sensor Science and Technology
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• v.6 no.3
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• pp.188-193
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• 1997

The lanthanum-modified lead titanate (PLT) thin films on (100) cleaved MgO single crystal substrate have been prepared by RF magnetron sputtering method using PbO-rich target with varing La contents. The substrate temperature, working pressure, $Ar/O_{2}$, and RF power density of PLT thin films were $580^{\circ}C$ 10mTorr, 10/1, and $1.7W/cm^{2}$, respectively. In these conditions, the c-axis growth and tetragonality of the PLT thin films decreased for addition of La content and the PLT thin films showed diffuse phase transition from high temperature XRD patterns. The infrared sensor was fabricated. The remanent polarization was above $1.71{\mu}C/cm^{2}$ and the pyroelectric voltage was above 500mV with 10:1 signal to noise ratio.

• Journal of the Microelectronics and Packaging Society
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• v.5 no.2
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• pp.59-64
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• 1998

Pt/SiO2/Si 기판구조위에 스크린인쇄법과 졸-겔법에 의해 (Pb, La)TiO3(PLT) 후막 과 박막을 도포시켜 $650^{\circ}C$후속열처리 온도에서 결정화한후 결정특성과 전기적 특성을 조사 하였다. $650^{\circ}C$ 온도에서 후속열처리된 PLT 시료의 경우 전형적인 perovskite 결정구조를 보 여주었다. SEM 단면형상으로부터 Pt 전극과 PLT막 사이에는 비교적 평활한 계면형상을 보여주었다. PLT 후막과 박막시료의 잔류분극(2Pr) 값은 약 1$\mu$C/cm2 으로각각 나타났으며 이와같이 후막 PLT시료에 비해 박막시료의 잔류분극값이 큰이유는 박막시료가 보다 양호 한 결정성을 지니기 때문이었다. 상온부근에서 후막과 박막시료의 초전계수값은 약 1.5nC/cm2.$^{\circ}C$와 4.0nC/cm2.$^{\circ}C$의 값을 각각 나타내었으며 누설전류의 크기는 약 0.3~0.8$\mu$ A/cm2의 비교적 양호한 누설전류 특성을 얻었다.

• Journal of the Institute of Electronics Engineers of Korea SD
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• v.38 no.3
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• pp.166-173
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• 2001

Hysteresis loops of the ferroelectric thin films such as PLZT(10/30/70), PLT(10) and PZT(30/70) was simulated using the field-dependent polarization model and compared to the measured loops. In case of PZT(30/70) thin film, as the real saturation or polarization at the applied voltage or larger than 5V appears slack and its value is quite different from the simulated one, it is deduced that the ferroelectric polarization of PZT(30/70) is generated not only by the pure dipoles but also by various electric charges. The drain current of quasi-MFISFET is expressed by using the square-law FET and field-dependent polarization models. The modeling results are analogous to the experimental values. The channel of quasi-MFISFET using PZT(30/70) forms more quickly compared to that of quasi-MFISFET using PLZT(10/30/70) or PLT(10) in the state of 'write' gate voltage of -10V. This may be because the decrease rate of the polarization in the PZT(30/70) thin film is 3~4 times more rapid than that of the polarization in the PLZT(10/30/70) or the PLT(10) thin film in the retention characteristics.

• Journal of the Institute of Electronics Engineers of Korea SD
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• v.38 no.3
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• pp.12-12
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• 2001

PLZT(10/30/70), PLT(10) 및 PZT(30/70) 와 같은 강유전체 박막의 이력곡선을 field-dependent polarization 모델을 이용하여 시뮬레이션하고, 측정한 실험적 결과와 비교, 분석하였다. PZT(30/70) 박막의 경우, 5V 이상의 인가전압에서 분극의 포화현상이 둔감하게 나타나고 시뮬레이션 값과의 차이도 심해 강유전체 분극이 순수한 dipole 외에도 다양한 전하의 영향을 받아 형성된다는 사실을 알 수 있다. 또, quasi-MFISFET 소자의 드레인 전류는 field-dependent polarization 모델의 강유전체 이력곡선에서 얻은 파라미터를 square-law FET 모델에 적용시켜 효과적으로 추출하였고, 모델링 결과는 실험값과 유사하였다. 그리고, quasi-MFISFET 소자의 gate 에 -10V의 ′write′ 전압을 인가한 상태에서 PZT(30/70) 박막을 사용한 경우, PLZT(10/30/70), PLT(10) 박막 보다 빨리 채널이 형성되었는데, 그 원인은 강유전체 박막에 따른 retention 특성에서 PZT(30/70) 박막의 분극 감소가 PLZT(10/30/70), PLT(10) 박막의 분극 감소 보다 약 3∼4 배 이상 크다는 점에서 찾을 수 있다.

• Journal of the Institute of Electronics Engineers of Korea SD
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• v.42 no.1
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• pp.1-8
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• 2005

We fabricate PLT(5) thin film on Pt/TiO/sub x/SiO₂/Si substrate by using sol-gel method and investigate leakage current, switching and retention properties. The leakage current density of PLT(5) thin film is 3.56×10/sup -7/A/㎠ at 4V. In the examination of switching properties, pulse voltage and load resistance were 2V～5V and 50Ω～3.3kΩ, respectively. Switching time has a tendency to decrease from 0.52㎲ to 0.14㎲ with the increase of pulse voltage, and also the time increases from 0.14㎲ to 13.7㎲ with the increase of load resistance. The activation energy obtained from the relation of applied pulse voltage and switching time is about 135kV/cm. The error of switched charge density between hysteresis loop and experiment of polarization switching is about 10%. Also, polarization in retention decreases as much as about 8% after l0/sup 5/s.

• Journal of the Korean Institute of Electrical and Electronic Material Engineers
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• v.11 no.2
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• pp.133-137
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• 1998

$(Pb_{0.72}La_{0.28})Ti_{0.93}O_3(PLT(28))$ thin films were fabricated by pulsed laser deposition. PLT films deposited on $Pt/Ti/SiO_2/Si$ at $600^{\circ}C$ had a preferred orientation in (111) plane and at $550^{\circ}C$ had a (100) preferred orientation. We found that (111) preferred oriented films had well grown normal to substrate surface. This PLT(28) thin films of $1{\mu}m$ thickness had dielectric properties of ${\varepsilon}_r$=1300, dielectric $loss{\fallingdotseq}0.03 $. and had charge storage density of 10 [${\mu}C/cm^2$] and leakage current density of less than $10^{-6}[A/cm^2]$ at 100[kV/cm]. These results indicated that the PLT(28) thin films fabricated by pulsed laser deposition are suitable for DRAM capacitor application.

• Journal of the Korean Institute of Telematics and Electronics D
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• v.36D no.1
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• pp.29-37
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• 1999

In this study, we have prepared PLT thin films having various La concentrations by using sol-gel method and studied on the effect of La concentration on the electrical properties of PLT thin films. As the La concentration increases from 5mol% to 28mol%, the dielectric constant at 10kHz increases from 428 to 761, while the loss tangent decreases from 0.063 to 0.024. Also, the leakage current density at 150kV/cm has a tendency to decrease from 6.96${\mu}A/cm^2$ to 0.79${\mu}A/cm^2$. In the result of hysteresis loops of PLT thin films, the remanent polariation and the coercive field decrease from 9.55${\mu}C/cm^2$ to 1.10${\mu}C/cm^2$ and from 46.4kV/cm to 13.7kV/cm, respectively. With the result of the fatigue test on the PLT thin films, we have found that the fatigue properties are improved remarkably as the La concentration increases from 5 mol% to 28mol%. In particular, the PLT28) has paraelectric phase and its charge storage clensity and leakage current density at 5V are 134fC/${\mu}cm^2$ and 1.01${\mu}A/cm^2$, respectively. The remanent polarization and coercive field of the PLT(10) film are 6.96${\mu}C/cm^2$ and 40.2kV/cm, respectively. After applying of $10^9$ square pulses with ${\pm}5V$, the remanent polarilzation of the PLT(10) film decreases about 20% from the initial state. In the results, we conclude that the 10mol% and the 28mol% La doped PLT thin films are very suitable for the capacitor dielectrics of new generation of DRAM and NVFRAM respecitively.

• Journal of the Institute of Electronics Engineers of Korea SD
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• v.39 no.3
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• pp.1-8
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• 2002

In order to study electric properties of (Pb$\_$0.9/La$\_$0.1/)Ti$\_$0.975/O$_3$(PLT (10)) films with varying excess lead concentration (7.5, 10, 12.5, 15 ㏖% excess lead), the PLT films were deposited by sol-gel process. DTA analyses reveal that the crystallization temperature of the precursor powers decreased with increasing amount of excess lead. XRD patterns of PLT reveal pure perovskite structure and the preferred orientation increased with increasing Pb content in the films. With increasing amount of excess P$\_$b/, the relative permittivity ($\xi$$\_$r/) increased and leakage current density at 100 ㎸/cm transformed 4.01$\times$10$\^$-5/, 2.42$\times$10$\^$-6/, 1.27$\times$10$\^$-6/, 1.56$\times$10$\^$-6/A/㎠ respectively. In the results of hysteresis loops measured at 166 kV/cm, the remanent polarization (P$\_$r/) and the coercive field (E$\_$c) are 6.36$\mu$C/cm and 58.7 ㎸/cm, respectively (at 12.5 ㏖% excess P$\_$b/) With increasing amount of excess Pb, the remanent polarization for PLT thin film degraded to about 44%, 27%, 15%, 16% of the initial value after 10$\^$9/ cycles./TEX>) With increasing amount of excess Pb, the remanent polarization for PLT thin film degraded to about 44%, 27%, 15%, 16% of the initial value after $10^{9}$ cycles.

• Journal of the Korean Crystal Growth and Crystal Technology
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• v.8 no.3
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• pp.468-473
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• 1998

Sol-gel법을 이용하여 PbTiO3에 La을 10mol% 도핑한 박막을 bare Si(100)-wafer 위에 스핀 코팅법을 이용하여 제조하였다. 제조된 박막의 열처리 온도에 따른 결정화 거동을 살펴보고, 씨앗층(seeding layer)을 도입하여 박막의 미세구조 및 배향성을 SEM과 XRD로 관찰하였다. 씨앗층없이 일반적으로 제조된 박막의 경우는 우선 배향성을 나타내지 않았으나, 씨앗층을 도입한 경우에는 씨앗층의 두께 및 열처리 시간에 따라 막의 배향성이 달라졌다.

• Korean Journal of Optics and Photonics
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• v.7 no.1
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• pp.44-50
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• 1996