• 제목/요약/키워드: Dielectric loss factor

검색결과 157건 처리시간 0.024초

BiTiO3 첨가에 따른 (Na0.5K0.5)NbO3 세라믹스의 구조적, 전기적 특성 (Structural and Electrical Properties of (Na0.5K0.5)NbO3 Ceramics with Addition of BiTiO3)

  • 이태호;김대영;조서현;정광호;이성갑
    • 전기학회논문지
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    • 제60권11호
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    • pp.2093-2096
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    • 2011
  • In this study, lead-free $(Na_{0.5}K_{0.5})NbO_3-BiTiO_3$ ceramics were fabricated by a conventional mixed oxide method. Structural and electrical properties of lead-free $(Na_{0.5}K_{0.5})NbO_3$ ceramics with the variation of $BiTiO_3$ were investigated. The results of X-ray diffraction analysis showed a typical polycrystalline perovskite structure without presence of the second phase in all specimens. Sintered density increased with an increasing of BTO and the specimen added with 0.07 mol% of $BiTiO_3$ showed the maximum value of 97.8%. Average grain size decreased and densification increased with an increasing of $BiTiO_3$ contents. The electromechanical coupling factor of the 0.01 mol% $BiTiO_3$ doped NKN specimens was 0.32. Dielectric constant, dielectric loss and Curie temperature of the 0.07 mol% $BiTiO_3$ doped NKN specimens were 1185, 0.145% and $400^{\circ}C$, respectively.

Two-Resonance Mode 방법용으로 제작된 고온초전도 평행판 사파이어 공진기의 마이크로파 특성 (Microwave Properties of HTS Parallel-Plate Sapphire Resonators Designed for the Two-Resonance Mode Method)

  • 정호상;양우일;이재훈;이상영
    • Progress in Superconductivity
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    • 제11권2호
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    • pp.106-111
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    • 2010
  • Sapphire resonators with $YBa_2Cu_3O_{7-\delta}$ (YBCO) endplates have provided a way to realize extremely high quality factor due to the extremely low dielectric loss of sapphire and conductive loss of YBCO films, which enables to measure the low surface resistance of superconductor films at microwave frequencies. We present microwave properties of HTS sapphire resonators designed for measuring the surface resistance of HTS films at millimeter-wave frequencies by using the two-resonance mode dielectric resonator method. Despite enhanced surface resistance ($R_S$) of YBCO films due to the quadratic frequency dependence of the $R_S$, the unloaded quality factor ($Q_0$) of the $TE_{021}$ mode sapphire resonator still appears to be well above $1\;{\times}\;10^6$ at a mm-wave frequency of 38 GHz at 10 K. However, it appears that the $TE_{012}$ mode $Q_0$ is unexpectedly low despite that the corresponding resonance peak looks uncoupled with parasitic modes. We discuss possible reasons for the unexpected results using the surface resistance at the $TE_{021}$, $TE_{012}$, and $TE_{011}$ mode frequencies.

소결온도에 따른 (Na0.465K0.465Bi0.07)(Nb0.93Ti0.07)O3-0.08MnO2 세라믹스의 구조적, 전기적 특성 (Structural and Electrical Properties of (Na0.465K0.465Bi0.07)(Nb0.93Ti0.07)O3-0.08MnO2 Ceramics with Variation of Sintering Temperature)

  • 이태호;여진호;이성갑
    • 한국전기전자재료학회논문지
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    • 제25권7호
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    • pp.506-510
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    • 2012
  • In this study, lead-free $(Na_{0.465}K_{0.465}Bi_{0.07})(Nb_{0.93}Ti_{0.07})O_3-0.08MnO_2$ ceramics were fabricated by conventional mixed oxide method. Structural and electrical properties of lead-free $(Na_{0.465}K_{0.465}Bi_{0.07})(Nb_{0.93}Ti_{0.07})O_3-0.08MnO_2$ ceramics with the variation of sintering temperature were investigated. As results of x-ray diffraction analysis, all specimens showed a typical polycrystalline perovskite structure without presence of the second phase. Sintered density increased with an increases of sintering temperature and the specimen sintered at $1,020^{\circ}C$ showed the maximum value of 4.5 $g/cm^3$. The average grain size of the $(Na_{0.465}K_{0.465}Bi_{0.07})(Nb_{0.93}Ti_{0.07})O_3-0.08MnO_2$ specimen sintered at $1,020^{\circ}C$ is about 0.83 ${\mu}m$. Electromechanical coupling factor, relative dielectric constant and dielectric loss of $(Na_{0.465}K_{0.465}Bi_{0.07})(Nb_{0.93}Ti_{0.07})O_3-0.08MnO_2$ specimens sintered at $1,020^{\circ}C$ were 0.252, 741 and 0.043% respectively.

X-Band 레이더를 위한 3-포트 서큘레이터 (3-Port Circulator for X-Band Radar)

  • 윤성현
    • 한국통신학회논문지
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    • 제40권2호
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    • pp.355-362
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    • 2015
  • 본 연구에서는 X-밴드 레이더에서 사용하는 9.385[GHz] 서큘레이터를 Y형 WR112 도파관속에 페라이트를 삽입하여 제작을 하였다. 페라이트 설계는 B/R(Below Resonance) 모드 방식을 사용하여, 페라이트 내부에서 전계 분포가 120도의 회전이 발생하는 조건과 페라이트의 내부의 직류 자계의 세기와 외부 자계의 세기를 계산하였다. 또한, 임피던스 정합을 포함하여 대역폭, 선택도, 삽입손실 등, 서큘레이터의 성능 향상을 위하여 두 개의 페라이트 사이에 같은 형태의 유전체를 삽입하였다. 최적의 페라이트 형태 및 유전체를 얻기 위하여 CST MWS를 이용하였다. 9.385[GHz]에서 시뮬레이션 결과는 정재파비 1.02, 분리도 -40dB, 삽입손실 0.2dB의 결과를 얻었고, 측정 결과는 정재파비 1.03, 분리도 -38dB, 삽입손실 1.2dB 이었다. 분리도, 정재파비는 시뮬레이션 결과와 잘 일치 하였지만, 삽입손실은 약 1dB 정도 크게 발생하였다.

다구찌 실험 계획법을 이용한 나선형 인덕터의 패턴드 그라운드 쉴드 최적 설계 연구 (Optimization of 'Patterned Ground Shield' of Spiral Inductor using Taguchi's Method)

  • 고재형;오상배;김동훈;김형석
    • 한국정보통신설비학회:학술대회논문집
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    • 한국정보통신설비학회 2007년도 학술대회
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    • pp.436-439
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    • 2007
  • This paper describes the optimization of PGS(Patterned Ground Shield) of 5.5 turns rectangular spiral inductor using Taguchi's method. PGS is decrease method of parasite component by silicon substrate among dielectric loss reduction method. By using the taguchi's method, each parameter is fixed upon that PGS high poison(A), slot spacing(B), strip width(C) and overlap turn number(D) of PGS design parameter. Then we verified that percentage contribution and design sensitivity analysis of each parameter and level by signal to noise ratio of larger-the-better type. We consider percentage contribution and design sensitivity of each parameter and level, and then verify that model of optimization for PGS is lower inductance decreasing ratio and higher Q-factor increasing ratio by EM simulation.

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Dependence of Q Factor on Surface Roughness in a Plasmonic Cavity

  • Kim, Yoon-Ho;Kwon, Soon-Hong;Ee, Ho-Seok;Hwang, Yongsop;No, You-Shin;Park, Hong-Gyu
    • Journal of the Optical Society of Korea
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    • 제20권1호
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    • pp.188-191
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    • 2016
  • We investigated surface-roughness-dependent optical loss in a plasmonic cavity consisting of a semiconductor nanodisk/silver nanopan structure. Numerical simulations show that the quality factors of plasmonic resonant modes significantly depend on the surface roughness of the dielectric-metal interface in the cavity structure. In the transverse-magnetic-like whispering-gallery plasmonic mode excited in a structure with disk diameter of 1000 nm, the total quality factor decreased from 260 to 130 with increasing root-mean-square (rms) surface roughness from 0 to 5 nm. This quantitative theoretical study shows that the smooth metal surface plays a critical role in high-performance plasmonic devices.

유리관의 유전 특성이 외부전극 형광램프에 미치는 영향 (Influence of Glass Dielectric Property on the External Electrode Fluorescent Lamps)

  • 신명주;정종문;김정현;김가을;이미란;유동근;구제환;홍병희;최은하;조광섭
    • 한국진공학회지
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    • 제16권5호
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    • pp.330-337
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    • 2007
  • 유전 장벽 방전이 특징인 외부전극 형광램프(External Electrode Fluorescent Lamp, EEFL)에서 유리재의 유전 특성인 유전상수 K와 유전손실 tan ${\delta}$가 램프에 미치는 영향을 조사하기 위하여 4 종류의 유리관을 사용하였다. 종래 일반적으로 사용되는 Borosilicate 유리재는 유전상수 $K=5.6{\sim}5.9$이고 유전 손실 tan ${\delta}=5.0{\times}10^{-3}{\sim}6.0{\times}10^{-3}$이다. Aluminosilicatae는 K=6.6이고 유전손실이 작은 tan ${\delta}=1{\times}10^{-4}$이다. Soda-lime 유리관은 유전상수가 큰 K=7.7이고, 유전 손실이 매우 큰 tan ${\delta}=1.37{\times}10^{-2}$이다. 유전 상수 K가 크면 외부전극 자체의 캐패시터를 크게 하여 방전 효율이 증가한다. 그러나 유전 손실이 크면 외부전극 자체의 전력 소모로 인하여 효율 저하와 핀홀 발생의 원인이 된다. 높은 유전상수 및 낮은 유전손실의 Aluminosilicate 외부전극 형광램프는 종래의 Borosilicate 외부전극 형광램프에 비하여 휘도와 효율이 $12{\sim}20%$ 증가하고, 핀홀에 매우 강하다. 유전상수와 유전손실이 큰 Soda-lime 외부전극 형광램프는 효율이 다소 낮고, 핀홀에도 매우 취약하다. 따라서 외부전극 형광램프는 유전상수 K가 크고 유전손실 tan ${\delta}$가 작은 유리관이 최적이다.

BST 후막의 가변 유전특성과 큐리온도에 관한 연구 (Tunable Dielectric Properties and Curie Temperature with BST Thick Films)

  • 김인성;송재성;민복기;전소현
    • 대한전기학회논문지:전기물성ㆍ응용부문C
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    • 제55권8호
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    • pp.392-398
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    • 2006
  • The properties of tunable dielectric materials on RF frequency band are important high tunability and low loss for RF variable devices, variable capacitor, phased array antenna and other components application. Various composite of BST(barium strontium titanate) ratio combined with other non-electrical active oxide ceramics have been formulated for such uses. We present the tunable properties and Curie temperature on BST thick films. The grain growth of the weight ratio of $BaTiO_3$ increased. This can be explained by the substitute $Sr^{2+}$ ion for $Ba^{2+}$ ion in the $BaTiO_3$ system. The Curie temperature was shifted to lower temperature with increasing $SrTiO_3$in the $BaTiO_3-SrTiO_3$ system, because of decreasing the lattice constant. Also, the dielectric constant, tunability and K-factor of $(Ba_xSr_{1-x})TiO_3$ at over the Curie temperature decreased, at over the $60^{\circ}C$ fixation, maximum dielectric constant at Curie temperature and hence sharper phase transformation occurred at Curie temperature. The result were interpreted as a process of internal stress relaxation resulting form the increase of $90^{\circ}$ domains induced the BST. As a result, It is concluded that over the Curie temperature, frequency response and DC field effect for the tunable properties of BST thick film are suppressed by the transition broadening. For the application of tunable devices, that the curie temperature was investigated to be increased.

Effect of Mn on Dielectric and Piezoelectric Properties of 71PMN-29PT [71Pb(Mg1/3Nb2/3)O3-29PbTiO3] Single Crystals and Polycrystalline Ceramics

  • Oh, Hyun-Taek;Joo, Hyun-Jae;Kim, Moon-Chan;Lee, Ho-Yong
    • 한국세라믹학회지
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    • 제55권2호
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    • pp.166-173
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    • 2018
  • In order to investigate the effect of Mn on the dielectric and piezoelectric properties of PMN-PT [$Pb(Mg_{1/3}Nb_{2/3})O_3-PbTiO_3$], four different types of 71PMN-29PT samples were prepared using the solid-state single crystal growth (SSCG) method: (1) Undoped single crystals, (2) undoped polycrystalline ceramics, (3) Mn-doped single crystals, and (4) Mn-doped polycrystalline ceramics. In the case of single crystals, the addition of 0.5 mol% Mn to PMN-PT decreased the dielectric constant ($K_3{^T}$), piezoelectric charge constant ($d_{33}$), and dielectric loss (tan ${\delta}$) by about 50%, but increased the coercive electric field ($E_C$) by 50% and the electromechanical quality factor ($Q_m$) by 500%, respectively. The addition of Mn to PMN-PT induced an internal bias electric field ($E_I$) and thus specimens changed from piezoelectrically soft-type to piezoelectrically hard-type. This Mn effect was more significant in single crystals than in ceramics. These results demonstrate that Mn-doped 71PMN-29PT single crystals, because they are piezoelectrically hard and simultaneously have high piezoelectric and electromechanical properties, have great potential for application in fields of SONAR transducers, high intensity focused ultrasound (HIFU), and ultrasonic motors.

Variation in optical, dielectric and sintering behavior of nanocrystalline NdBa2NbO6

  • Mathai, Kumpamthanath Chacko;Vidya, Sukumariamma;Solomon, Sam;Thomas, Jijimon Kumpukattu
    • Advances in materials Research
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    • 제2권2호
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    • pp.77-91
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    • 2013
  • High quality nanoparticles of neodymium barium niobium ($NdBa_2NbO_6$) perovskites have been synthesized using an auto ignition combustion technique for the first time. The nanoparticles thus obtained have been characterized by powder X-ray diffraction, thermo gravimetric analysis, differential thermal analysis, Fourier transform infrared spectroscopy, Raman spectroscopy and transmission electron microscopy. UV-Visible absorption and photoluminescence spectra of the samples are also recorded. The structural analysis shows that the nano powder is phase pure with the average particle size of 35 nm. The band gap determined for $NdBa_2NbO_6$ is 3.9 eV which corresponds to UV-radiation for optical inter band transition with a wavelength of 370nm. The nanopowder could be sintered to 96% of the theoretical density at $1325^{\circ}C$ for 2h. The ultrafine cuboidal nature of nanopowders with fewer degree of agglomeration improved the sinterability for compactness at relatively lower temperature and time. During the sintering process the wide band gap semiconducting behavior diminishes and the material turns to a high permittivity dielectric. The microstructure of the sintered surface was examined using scanning electron microscopy. The striking value of dielectric constant ${\varepsilon}_r=43$, loss factor tan ${\delta}=1.97{\times}10^{-4}$ and the observed band gap value make it suitable for many dielectric devices.