• Title/Summary/Keyword: Permittivity

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Formation Rate of Tetragonal BaTiO3 Powder by Hydrothermal Synthesis and its Dielectric Property (수열합성법에 의한 정방정 BaTiO3 분말의 생성속도 및 유전특성)

  • 이종현;최용각;원창환;김채성
    • Journal of the Korean Ceramic Society
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    • v.39 no.7
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    • pp.628-634
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    • 2002
  • Formation rate of tetragonal BaTiO$_3$powder by hydrothermal synthesis and its dielectric property were studied. Submicron tetragonal BaTiO$_3$ powders were prepared hydrothermally, using Ba(OH)$_2$.8$H_2O$, TiO$_2$(anatase) and KOH as starting chemicals. Characterization via X-ray diffractometry, field emission scanning electron microscopy confirmed that increasing calcination temperatures(from 1100 to 130$0^{\circ}C$) promotes the formation of tetragonal BaTiO$_3$. Tetragonal BaTiO$_3$ ceramics, obtained by calcining at 1200 for 3 h after hydrothermal synthesis at 200 for 168 h, exhibited submicron size of 0.5 ~ 0.7 ${\mu}{\textrm}{m}$ and high relative permittivity.

Growth and Characterization of $ACu_3Ti_4O_{12}$(A=Ca, Sr) Single Crystals

  • Yoo, Sang-Im;Sangdon Yang;Geomyung Shin;Wee, Seong-Hun;Park, Hyun-Min
    • Proceedings of the Korea Crystallographic Association Conference
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    • 2003.05a
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    • pp.19-19
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    • 2003
  • A cubic perovskite-type CaCu₃Ti₄O/sub 12/ compound has recently drawn a great attention because of an extraordinary high permittivity (~10⁴ at 1 kHz) at room temperature and its near temperature-independence over a wide temperature region, and thus numerous literature have been reported on CCTO polycrytalline ceramics and thin films. However, only a few literature have been reported on the CCTO single due to the lack of information about the CCTO primary phase field. On the basis of our recent experimental determination of the CCTO primary phase field, we could grow ACu₃Ti₄O/sub 12/(A=Ca, Sr) single crystals using both top-seeded solution growth and flux growth methods. This presentation will include three major parts. In part I, the thermal decomposition reaction of CCTO and its primary phase field in the CaO-CuO-TiO₂ ternary system will be presented. Detailed growth conditions of ACu₃Ti₄O/sub 12/(A=Ca, Sr) single crystals and characteristics of as-grown crystals will be followed in Part II. Part III will be comprised of dielectric properties of as-grown ACu₃Ti₄O/sub 12/(A=Ca, Sr) single crystals. Our experimental results will be compared with those of previous reports for discussion.

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Electrical Properties of $C_{22}$-Quinolium(TCNQ) Langmuir-Blodgett Films Depending on the Frequency ($C_{22}$-Quinolium(TCNQ) LB 막의 주파수에 따른 전기적 특성)

  • Lee, S.K.;You, D.S.;Kim, T.W.;Kim, Y.K.;Kwon, Y.S.;Kang, D.Y.
    • Proceedings of the KIEE Conference
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    • 1994.07b
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    • pp.1289-1291
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    • 1994
  • Dielectric properties of $C_{22}$-Quinolium(TCNQ) Langmuir-Blodgett (LB) films were studied as a function of frequency(10Hz-13MHz) and annealing temperature($20{\sim}240^{\circ}C$). A complex dielectric constant ${\epsilon}^*={\epsilon}'-i{\epsilon}"$, in general, shows the frequency dependence of orientational polarization in the measured frequency range. A dielectric permittivity ${\epsilon}'$ at 10Hz is around 8.2 and decreases very slowly as the frequency increases up to 1 MHz, and then suddenly drops above this frequency, while a dielectric loss factor ${\epsilon}"$ reaches a maximum near 1 MHz. Its annealing temperature dependence at 10Hz shows that ${\epsilon}'$ and ${\epsilon}"$ increase as the temperature increases upto $180^{\circ}C$, even though there is a little drop near $120{\sim}160^{\circ}C$. Both ${\epsilon}'$ and ${\epsilon}"$ drop quickly above $180^{\circ}C$. which may be thought of a destruction of the LB films. Another fact of the annealing temperature dependence of the dielectric constant is an occurrence of the new dielectric dispersion below 100Hz. This low frequency dispersion is getting clear above $80^{\circ}C$.

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A Study on the Simulation of Complex Permittivities of Carbon Black/Epoxy Composites at a High Frequency Band (고주파에서의 카본 블랙/에폭시 복합재료 복소유전율 모사에 대한 연구)

  • Kim Tae-Wook;Kim Chun-Gon;Kim Jin-Bong
    • Composites Research
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    • v.18 no.3
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    • pp.14-20
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    • 2005
  • This paper presents a study on the permittivities of the carbon black/epoxy composite at microwave frequency. The measurements were performed at the frequency band of $1\;GHz\~18\;GHz$. The experimental data show that the complex permittivities of composites depend strongly on the natures and concentrations of the carbon black dispersion. The frequency characteristics of dielectric constants and ac conductivities of composites show the good conformity with descriptions of the percolation theory, satisfying the general scaling relation. The measuring frequency band is over the critical frequency, below that the ac conductivities of composites are constant to the frequency. The values of dielectric constants and ac conductivities have consistent relationships with the carbon black concentration. The A new scheme, that is a branch of Lichtenecker-Rother formula, is proposed to obtain a mixing law to describe the complex permittivities of the composites as function frequency and concentration of carbon black.

The effects of the composition and the lower electrode on the properties of PZT thin films prepared by Sol-Gel method (Sol-Gel 법으로 제작된 PZT 박막의 전기적 성질에 조성과 하부전극이 미치는 영향)

  • 이정기;윤영섭
    • Journal of the Korean Institute of Telematics and Electronics A
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    • v.32A no.7
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    • pp.77-84
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    • 1995
  • We studied the effects of the Zr/Ti ration and the bottom electrode (Pt or ITO) on the electrical properties of PZT thin films prepared by sol-gel method. Their permittivities and tagent losses with the variation of frequencies were measured by the LCR meter and their maximum polarizations, remanent polarizations, and coercive fields were obtained from the hysteresis loops measured by the Sawyer-Tower circuit. For the PZT thin film of the Zr/Ti ration of 53/47, permittivity at 10kHz, coercive field, maximum and remanent polarizations ere measured as 952, 20.7kV/cm, 10.43${\mu}C/cm^{2}$ and 4.3${\mu}C/cm^{2}$, respectively. For the film of the Zr/Ti ration of 25/75, coercive field, maximum and remanent polarizations were measured as 33.12kV/cm, 5.59${\mu}C/cm^{2}$ and 1.5${\mu}C/cm^{2}$, respectively. For the film of the Zr/Ti ratio of 75/25, they were measured as 23.8kV/cm, 7.45${\mu}C/cm^{2}$, and 3.5${\mu}C/cm^{2}$, repectively. Our investigation into the effects of the lower electrode on the electrical properties of PZT films showed the following results. The permittivities of the PZT films deposited on the ITO electrode decreased more quickly than those of the PZT films on the Pt electrode. The tangent losses of the former films increased more quickly than those of the latter. These may be due to the degradation of the quality of the interface between the electrode and the film, which results from the diffusion of Pb. It is also noticeable that permittivities and tangent losses of the PZT films deposited on the ITO electrode varied differently with the Zr/Ti ratio. This may indicate that the quality of the interface between the electrode and the film changes with the Zr/Ti ration of the PZT film.

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Modified Microwave Radio-thermometer for Measuring Temperature of Living Body (생체의 온도 측정을 위한 수정된 마이크로파 라디오-써모미터)

  • Kim Tae-Woo;Cho Tae-Kyung;Park Byoung-Soo
    • Journal of the Institute of Electronics Engineers of Korea SC
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    • v.42 no.2 s.302
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    • pp.27-32
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    • 2005
  • This paper presents a modified microwave radio-thermometer (MRTM) with material characteristic estimator and multiple temperature conversion tables to measure subcutaneous temperature of a living body This estimator provides a temperature retrieval unit with the data of material characteristics such as permittivity, conductivity, thickness and geometry of the living body. The temperature retrieval unit with multiple temperature conversion tables can select one of the tables and computes temperature value corresponding to measured radiation power. In the experiments, it was shown that the MRTM could reduce measurement errors of about $0.82^{\circ}C\;to\;7.68^{\circ}C$ for the cases of distilled water and mixed liquid at the temperature of $37^{\circ}C$.

A Study on TE Scattering by a Conductive Strip Grating Over Two Dielectric Layers (2개 유전체층 위의 완전도체띠 격자구조에 의한 TE 산란에 관한 연구)

  • Yoon, Uei-Joong
    • The Journal of the Institute of Internet, Broadcasting and Communication
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    • v.16 no.2
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    • pp.87-92
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    • 2016
  • In this paper, the solutions of TE(transverse electric) scattering problems by a conductive strip grating over two dielectric layers are analyzed by applying the PMM(point matching method) known as a numerical method of electromagnetic field. The boundary conditions are applied to obtain the unknown field coefficients, the scattered electromagnetic fields are expanded in a series of Floquet mode functions, and the conductive boundary condition apply to analysis of conducting strip. The most normalized reflected and transmitted powers having a sharp variations are scattered in direction of the other angles except incident angle. The numerical results for the normalized reflected and transmitted powers are analyzed by according as the width and spacing of conductive strip, incident angles, and the relative permittivity and thickness of the two dielectric layers. To confirm the validity of this paper, the numerical results of presented structure are shown in good agreement compared to those of the existing papers.

A Study on TE Scattering by a Conductive Strip Grating Between a Double Dielectric Layer (2중 유전체층 사이의 완전도체띠 격자구조에 의한 TE 산란에 관한 연구)

  • Yoon, Uei-Joong
    • The Journal of the Institute of Internet, Broadcasting and Communication
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    • v.17 no.2
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    • pp.83-88
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    • 2017
  • In this paper, TE(transverse electric) scattering problems by a conductive strip grating between a double dielectric layer are analyzed by applying the PMM(point matching method) known as a numerical method of electromagnetic fileld. The boundary conditions are applied to obtain the unknown field coefficients, the scattered electromagnetic fields are expanded in a series of Floquet mode functions, and the conductive boundary condition is applied to analysis of the conductive strip. The numerical results for the normalized reflected and transmitted power are analyzed by according as the width and spacing of conductive strip, the relative permittivity and thickness of the double dielectric layers, and incident angles. The most normalized reflected powers of the sharp variations in minimum values are scattered in direction of the other angles except incident angle. The numerical results for the presented structure of this paper are shown in good agreement compared to those of the existing papers.

Wideband Annular Ring Slot Microstrip Antenna with Concentric Radiating Structure (동심원 복사구조를 갖는 광대역 원형 링슬롯 마이크로스트립 안테나)

  • Shin, Ho-Sub;Kim, Nam;Rhee, Seung-Yeop;Ahn, Bierng-Chearl
    • Journal of the Institute of Electronics Engineers of Korea TC
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    • v.40 no.9
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    • pp.384-391
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    • 2003
  • The wideband annular ring slot antenna with concentric radiating structure and low impedance feedline has been presented. This antenna has been analyzed in compensation for FR-4 substrate with relative permittivity 4.3 and thickness 1 mm. As the measured 10 dB impedance bandwidth of the proposed antenna is 127.2%(2.17∼9.76 GHz), its bandwidth is much broader than maximum 82% bandwidth of a conventional annular ring slot antenna. Experimental results from 2 to 10 GHz are shown to be in good agreement with the simulation. And this antenna has a high gain above 4 dBi from 2 GHz to 10 GHz as well as a 24% size reduction and 42% area reduction than a circular slot antenna.

The Design of Ring Resonator with Considering Effect of Coupling Gap (결합 갭의 영향을 고려한 링 공진기의 설계)

  • Oh, Teresa;Kim, Heung-Soo
    • Journal of the Korean Institute of Telematics and Electronics D
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    • v.36D no.8
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    • pp.27-35
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    • 1999
  • A radius of ring resonator is determined by the resonant frequency. Resonant frequencies of resonators with the circumference which is integer times of wave length are not same the expected. In this paper, we suggest the design method of a ring resonator with coupling gap, which has the resonant frequency of desire. The equation which can make reduction of the radius of the resonators depending on the gap space is derived by the method of transmission line analysis. The criterion is suggested to determine the radius of the resonator in accordance with relative permittivity. A ring resonator by the proposed method is as small as one-third of basic ring in size and it has the resonant frequency of desire. T-type coupling line is designed to obtain large attenuation of $S_{11}$ at pass-band. These coupling line capacitances are very lower than the gap capacitances, it does not affect the resonant frequency.

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