• 제목/요약/키워드: Waveguide

검색결과 1,899건 처리시간 0.041초

주기적으로 분리된 광도파로로 구성된 모드 크기 변환기의 설계 및 분석 (Design and analysis of a mode size converter composed of periodically segmented taper waveguide)

  • 박보근;정영철
    • 한국광학회지
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    • 제15권1호
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    • pp.22-27
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    • 2004
  • 본 논문에서는 광도파로와 광섬유사이에서 광손실을 줄이기 위한 모드 크기 변환기를 설계하였다. 설계된 모드 크기 변환기는 주기적으로 분리된 테이퍼 광도파로로 구성된 모드 크기 변환기이며, 공정상의 적용이 용이한 수평 테이퍼 구조를 선택하였다. 높이와 폭이 3$\mu\textrm{m}$${\times}$3$\mu\textrm{m}$이며 1.5%실리카 광도파로의 경우 파장이 1550nm 파장에서 최적의 모드 크기 변환기 설계 파라미터는 테이퍼 영역의 길이가 500$\mu\textrm{m}$이고, 분리된 광도파로의 길이는 5$\mu\textrm{m}$이며, 주기의 Duty-Cycle은 0.95, 광도파로와 광섬유의 접속면에서의 폭은 1.3$\mu\textrm{m}$이였다. 이 때 결합손실은 0.33㏈/point로 광섬유와 광도파로를 직접 연결할 때 보다 1.27 ㏈/point가 감소하였다.

불연속을 보상한 Q밴드 모드 변환기의 설계 및 도파관 혼합기 모듈 제작에의 응용 (Design of Q-band Mode Converter with the Discontinuity Compensation and Its Application to Waveguide Mixer Module)

  • 한상은;이종환;염경환
    • 한국전자파학회논문지
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    • 제14권11호
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    • pp.1198-1206
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    • 2003
  • 본 논문에서는 도파관 대 마이크로스트립 모드 변환기를 설계하고 이를 바탕으로 도파관 혼합기 모듈을 제작 측정하였다. 설계된 모드 변환기는 반사손실을 최소화하기 위하여 50 $\Omega$ 마이크로스트립 라인의 패턴을 변화시킴으로서 도파관 내 릿지와 마이크로스트립 사이의 불연속부분의 영향을 보상하였다. 이렇게 제작된 모드 변환기를 사용함으로써 밀리미터파 대역에서 개발된 MMIC 칩을 저 손실 guiding이 가능하도록 도파관 내에 장착시켜 시스템으로의 적용이 가능하도록 하였다. 제작된 도파관 혼합기 모듈의 측정 결과, 제공된 MMIC에서 얻어진 혼합기의 사양의 성능저하가 거의 없음을 알 수 있었다.

다층 구조 도파관 소자 단면에의 무반사 코팅 설계 (Design of antireflection coationgs on the facets of a multilayered structure waveguide device)

  • 김용곤;김부균;주흥로
    • 한국통신학회논문지
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    • 제21권7호
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    • pp.1850-1860
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    • 1996
  • We present the results for the design ofantireflection (AR) coatings on facets of a multilayered structure waveguide device. The method, whose results agree very well with the reusults of the rigorous method in the case of a symmetric three layer structure deveice, is extended for the design of AR coatings on the facets of a multilayered structure waveguide device. the field profile in a multilayered structure waveguide necessary for the use of the extended method is obtained from the transfer matrix method. The virtual four layered structure method (VFLM) is proposed to reduce the time for the design ofAR coatings because the time for the design of AR coatings using the extended method increases as the number of layers increases. The optimum coating parameters and tolerance mapsfor two different six layered waveguide devices in Ref. [9] and [10] are obtained using the extendedmethod and the VFLM,and for the three different cases approximated as three layered waveguide devices to compare the results of each case. The results of the VFLM are similar to those of the extended methodcompared to those of the three layered structure waveguide. The main reason for the above results is that the field profile in the device calculated usingthe VFLM is similar to that calculated using the extended method compared to that for three layered structure wavegjide. We conclude that the extended method or VFLM should be used for the design of AR coatings on facets of a deice required for the facet reflectivity less than 10$^{-3}$ such as a semiconductor otical amplifier.

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Bus-waveguide-width Dependence of Evanescent Wave Coupling in a Microring Resonator

  • Son, Seong-Jin;Kim, Suyeon;Yu, Nan Ei;Ko, Do-Kyeong
    • Current Optics and Photonics
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    • 제5권5호
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    • pp.538-543
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    • 2021
  • The evanescent wave coupling of a microring resonator is controlled by changing the gap distance between the bus waveguide and the microring waveguide. However, the interdependence of the bus waveguide's width and the coupling is not well understood. In this paper, we investigate the dependence of coupling strength on the bus waveguide's width. The strength of the evanescent wave coupling is analytically calculated using coupled-mode theory (CMT) and numerically calculated by three-dimensional finite-difference-time-domain (FDTD) simulation. The analytic and numerical simulation results show that the phase-matching condition in evanescent wave coupling does not provide maximum coupling strength, because both phase-matching and mode confinement influence the coupling. The analytic and simulation results for the evanescent coupling correspond to the experimental results. The optimized bus-waveguide width that provides maximum coupling strength results in intrinsic quality factors of up to 1.3 × 106. This study provides reliable guidance for the design of microring resonators, depending on various applications.

구형 유전체판이 삽입된 구형도파관 이상기에 관한 연구 (A Study on the Rectangular Waveguide Phase-Shifter Partially Loaded with a Rectangular Dielectric Slab)

  • 박병우;이상설
    • 한국통신학회논문지
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    • 제15권10호
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    • pp.850-856
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    • 1990
  • Generally, the waveguide phase-shifter has been analyzed by the modal expansion method. We can not apply this method in the case which is difficult to choose a nenerating function. In this paper, we are analyzed the rectangular waveguide phase shifter using the perturbation method. When the depth of dielectric slab is smaller then one half of the waveguide height, the experimental results are well agreed with the calculated values by this method.

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구형 도파관으로 차폐된 코플래너 도파관 해석 (Analysis of the Coplanar Waveguide Shielded by Rectangular Waveguide)

  • 황정섭;이상설
    • 전자공학회논문지A
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    • 제30A권7호
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    • pp.19-25
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    • 1993
  • By using the point matching method, the coplanar waveguide shielded by the rectangular waveguide has been analyzed. The particular potential solution of C.P.W has been obtained from the boundary condition by using the point matching method. The line capacitance has been obtained from the total charge of the center conductor per length. The effective dielectric constant and the line impedance have been obtained from the line capacitance of C.P.W.

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Waveguide Optical Matrix 용 졸-겔 코팅졸의 OH 함량 제어 (Control of Hydroxyl Group Content in Sol-Gel-Derived Sols for Waveguide Optical Matrix)

  • 안복엽;석상일;김주현;권정오
    • 한국재료학회:학술대회논문집
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    • 한국재료학회 2003년도 춘계학술발표강연 및 논문개요집
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    • pp.55-55
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    • 2003
  • Recently, with the rapid development of the waveguide division multiplexing (WDM) systems for large capacity and flexibility of information network, the broad band 1.5$\mu\textrm{m}$ erbium-doped waveguide amplifier (EDWA) become important. The main factors affecting the performance of sol-gel-based waveguides are non-radiative relaxation channels due to rare-earth concentration quenching and to vibration of the OH groups Therefore, the sol-gel process has to be carefully controlled in order to minimize the residual OH content.

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주기경계를 갖는 지파 마이크로파 도파관의 연구 (A Study of Slow Wave Microwave Waveguide on Period Boundary)

  • 김원섭
    • 전기학회논문지P
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    • 제58권4호
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    • pp.461-464
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    • 2009
  • The characteristics of slow wave structure employed for backward wave oscillators expected to be a high power microwave source are studied analyytically. The slow wave structure is a sinusoidally corrugated wall waveguide. The waveguide is designed and fabricated by cast aluminun. The dispersion relation and transmitted characteristics for microwaves are measured in the air. There exist literatures on high efficiency of enhanced radiation from backward wave oscillators involving plasma studied experimentally.

Optimal Design of Dielectric-Filled Plasmonic Slot Waveguide with Genetic Algorithm

  • Kim, Daekeun;Jung, Jaehoon
    • Journal of the Optical Society of Korea
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    • 제16권1호
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    • pp.70-75
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    • 2012
  • An optimization methodology for designing a dielectric-filled plasmonic slot waveguide is presented. The genetic algorithm combined with a rigorous analysis based on the finite element method is used to optimize a nano-scaled plasmonic slot waveguide to have high mode confinement and a long propagation length, for which the objective function is defined as a figure of merit combining both propagation parameters.

Operational Properties of Ridge Waveguide Lasers with Laterally Tapered Waveguides for Monolithic Integration

  • Kwon, Oh-Kee;Kim, Ki-Soo;Sim, Jae-Sik;Baek, Yong-Soon
    • ETRI Journal
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    • 제29권6호
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    • pp.811-813
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    • 2007
  • We report on a ridge waveguide laser diode with laterally tapered waveguides fabricated in a single growing step using a double patterning method. In this structure, nearly constant output power is obtained with the change of the lower tapered waveguide width, and the facet power ratio of 1.4 to 1.5 is observed over the current range. The asymmetric facet power property is also investigated.

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