• 제목/요약/키워드: spontaneous polarization

검색결과 84건 처리시간 0.021초

광대역 ASE 광원과 PI-RSOA를 이용한 WDM-PON 시스템에서의 방송 신호 전송 (Broadcast Signal Transmission on a WDM-PON System Using a Polarization Independent RSOA and a Broadband ASE Light Source)

  • 오영국;이혁재
    • 한국광학회지
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    • 제23권6호
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    • pp.264-268
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    • 2012
  • 본 논문에서는 파장분할 다중방식의 수동형 광 가입자망(WDM-PON: Wavelength Division Multiplexing - Passive Optical Network)에서 매우 구조가 간단하고 저비용으로 구현 가능한 방송신호 전송 방법을 제안한다. 이는 하나의 광대역 증폭된 자발 광원(Amplified Spontaneous Emission: ASE)과 편광 독립 반사형 반도체 광 증폭기(Polarization Independent-Reflective Semiconductor Optical Amplifier: PI-RSOA) 만으로 구현이 가능하기 때문이다. 채널당 1.25 Gb/s 속도에서 24개의 가입자 채널에 대해 30 Km 이상의 방송 신호 전송 시, 무오류(error-free) 성능을 갖는 것을 실험적으로 증명하였다.

PZT계의 정방정상과 능면체정상의 경계조성에 대한 기계적 응력과 전기장의 영향 : 열역학적 고찰 (The Effect of Mechanical Stress and Electric Field on the Morphotropic Tetragonal and Rhombohedr Phase Boundary in PZT System : Thermodynamic Consideration)

  • 천채일;김호기
    • 한국세라믹학회지
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    • 제30권10호
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    • pp.859-865
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    • 1993
  • Morphotropic tetragonal and rhombohederal phase boundary(MPB) in PZT system was calculated and the effect of mechanical stress and electric field on the MPB was examined using phenomenological thermodynamic theory proposed by Devonshire. Mechanical stress and electric field was calculated to change free energies of phases and shift MPB. The stable composition range of the phase, of which spontaneous strain and spontaneous polarization aligned to the direction of tensile stress or electirc field, was expanded.

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강유전체 분극 이력곡선의 측정 정밀도 향상 (Improvement of Precision in Ferroelectric Polarization Hysteresis Measurement)

  • 박재환
    • 마이크로전자및패키징학회지
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    • 제30권3호
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    • pp.51-55
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    • 2023
  • 강유전체 분극 이력곡선의 측정은 강유전체의 구조와 유전특성을 전반적으로 평가하고 해석하는 중요한 수단이다. 강유전체 시편에 저항성분이 포함될 경우 자발분극의 측정 값에 오차가 포함된다. 분극을 측정하는 전기적 회로를 구성할 때, 시편에 포함된 저항성분에 대응하는 외부 저항을 적절히 활용함으로서 시편의 저항성 손실에 의한 오차를 배제하고 내부에 유도된 강유전체 분극의 크기를 정확하게 측정할 수 있었다. 이와 같은 정확한 분극 이력곡선의 평가를 통하여 강유전체 내부의 이온의 변위 및 유전특성을 보다 정확하게 평가할 수 있을 것으로 기대된다.

열자극 탈분극전류 방법에 의한 BaTiO3의 분극 특성 연구 (Study on Polarization Properties of BaTiO3by Using Thermally Stimulated Depolarization Current)

  • 송호준;이용렬;박영준
    • 한국재료학회지
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    • 제12권8호
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    • pp.613-616
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    • 2002
  • The polarization properties of $BaTiO_3$ were investigated by using thermally stimulated depolarization current (TSDC) technique. Two peaks were observed at about 400 K (peak A) and 435 K (peak B) from TSDC spectra obtained from the temperature range of 280-500 K. Peak A shows a sharp decrease of TSDC due to extinction of spontaneous polarization above the phase transition temperature of $BaTiO_3$. The values of activation energy of peak A and peak B were calculated to be 0.70 eV and 0.87 eV respectively. From the results of TSDC measurement with a variation of polarizing electric field strength, we found that saturation of total current of TSDC was started from 3kV/cm. However, the amount of total current of TSDC was not affected by the variation of polarizing time.

Development of Spontaneous Polarization of Epitaxial Iron-Excess Gallium Ferrite Thin Films

  • Oh, S.H.;Shin, R.H.;Lee, J.H.;Jo, W.;Lefevre, C.;Roulland, F.;Thomasson, A.;Meny, C.;Viart, N.
    • 한국자기학회:학술대회 개요집
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    • 한국자기학회 2012년도 임시총회 및 하계학술연구발표회
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    • pp.121-122
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    • 2012
  • Iron-excess gallium ferrite, $Ga_{0.6}Fe_{1.4}O_3$ (GFO), is known to have room-temperature ferromagnetic phases and potentially exhibit ferroelectricity as well [1]. But, leaky polarization-electric field (PE) hysteresis curves of the GFO thin film are hurdle to prove its spontaneous polarization, in other words, ferroelecticity. One of the reasons that the GFO films have leaky PE hysteresis loop is carrier hopping between $Fe^{2+}$ and $Fe^{3+}$ sites due to oxygen deficiency. We focus on reducing conducting current by substituting divalent cations at $Fe^{2+}$ sites. GFO thin films were grown epitaxially along b-axis normal to $SrRuO_3/SrTiO_3$ (111) substrates by pulsed laser deposition. Current density of the ion-substituted GFO thin films was reduced by $10^3$ or more. Ferroelectric properties of the ion-substituted GFO thin films were measured using macroscopic and microscopic schemes. In particular, local ferroelectric properties of the GFO thin films were exhibited and their remnant polarization and piezoelectric d33 coefficient were obtained.

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복굴절이 큰 광섬유에 형성된 장주기 광섬유 격자를 이용한 파장 스위칭 가능한 광섬유 고리형 레이저 (Wavelength-Switchable Fiber Ring Laser Employing a Long-Period Fiber Grating Inscribed on a High Birefringent Fiber)

  • 이용욱
    • 전기학회논문지
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    • 제56권11호
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    • pp.1995-1997
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    • 2007
  • In this paper we propose a wavelength-switchable fiber ring laser that employs a polarization-dependent fiber band stop filter. The fiber filter was fabricated by inscribing a long-period fiber grating on a high birefringent fiber. Dual-wavelength switching operation was accomplished by controlling the rotatable linear polarizer which rotated the polarization plane of the light circulating through the fiber laser cavity. The amplitude variation of both laser lines was measured to be less than 0.5 dB and the signal-to-amplified spontaneous emission ratio was more than 55 dB.

성분에 따른 $Pb(Zr_xTi_{1-x})O_3$세라믹스의 Dynamic 초전 특성과 그 주파수 의존성 (Dynamic Pyroelectric Properties and Their Frequency Dependences of $Pb(Zr_xTi_{1-x})O_3$ Ceramics with Various Compositions)

  • 민경진;윤영섭
    • 대한전자공학회:학술대회논문집
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    • 대한전자공학회 1998년도 추계종합학술대회 논문집
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    • pp.609-612
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    • 1998
  • Pyroelectric properties of rhombohedral $Pb(ZrxTi_1-x)O_3ceramics$ with various Zr/Ti ratios of 84/16, 87/13, 90/10, and 93/7 are investigated using dynamic method. The response characteristics of PZT samples are examined by considering frequency dispersion. Since the reorientation of the grain does not the influence on the increase of frequency at low frequency (2~200Hz), the maximum pyroelectric response can be obtained with the change of spontaneous polarization. However, the pyroelectric response of PZT samples could be reduced as the spontaneous polarization decreases due to the restrain of the reorientation of the grain with the increasing of requency at high frequency (200~2000Hz). We have obtained the good pyroelectric response in the PZT sample having 84/16 Zr/Ti ratio, then the pyroelectric coefficient (${\gamma}$) and the figure of merit (FV) were $17.3nC/\textrm{cm}^2K$ and 2.28$\times$10-11Ccm/J, respectively. The noise equivalent power (NEP), the detectivity (D*) were 1.21$\times$10-7W/Hz$\frac{1}{2}$ and 8.26$\times$106cmHz$\frac{1}{2}$/W, respectively.

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