• 제목/요약/키워드: intermediate coupling layer

검색결과 9건 처리시간 0.016초

중간 결합층이 적층된 측면연마 광섬유 결합기의 해석 및 결합효율 개선 (Analysis of side-polished fiber couplers with an intermediate-coupling layer and improvement of their coupling efficiency)

  • 손경락;김광택
    • 한국광학회지
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    • 제15권1호
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    • pp.28-33
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    • 2004
  • 상부 도파로와 중간 결합층이 적층된 단일모드 광섬유를 기본구조로 하는 측면 연마 광섬유 결합기를 상호 광 결합이 일어나는 영역을 다층막 도파로로 등가화하여 결합 효율을 해석하였다. 다층막 구조에서 중간 결합층의 유무에 따른 반사도를 계산하여 상부 도파로의 굴절률의 함수로 도시하였고, 상부 도파로의 굴절률이 광섬유 코어의 굴절률보다 클 경우 중간 결합층의 조건에 의해서 광 결합이 증가되어짐을 보였다. 리튬나오베이트를 상부 도파로로 가지는 결합기의 실험결과를 톤해 이론적 해석의 타당함을 보였고 계산 결과와 일치함을 보였다.

측면 연마 광섬유 결합기를 이용한 파장분할 다중화 채널분리 필터 (Wavelength-division multiplexing channel isolation filter using a side-polished fiber coupler)

  • 손경락;김광택;송재원
    • 한국광학회지
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    • 제13권6호
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    • pp.461-466
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    • 2002
  • 파장분할 다중화 시스템의 다중 채널분리 필터가 측면연마 광섬유 결합기를 이용한 빗살필터로 구현됨을 제안하였다 단일 모드 광섬유의 기본모드와 결합하는 상부 평면 도파로의 모드가 고차일수록 광 전력전달 효율은 낮아지는데, 두 도파로 사이 에 중간 결합층을 삽입함으로서 개선시킬 수 있고 최적화 조건에서 20dB 이상의 채널간 소멸비를 얻을 수 있음을 보였다. 200fm두께의 리튬나오베이트를 상부 평면 도파로로 적용한 경우 4m의 채널간격을 가지는 빗살필터 특성을 얻었으며, 중간 결합층의 두께가 1 Um일 때 굴절률이 1.52-1.53 범위에서 최대 광 전력전달이 일어남을 관측하였고 빔 전파 방법을 이용하여 계산한 결과와 거의 일치함을 보였다.

얇은 중간 금속층을 포함한 측면 연마 광섬유 결합기를 이용한 편광 분리기 (Polarization Splitter Made of the Side-Polished Fiber Coupler Including a thin Metal Intermediate Layer)

  • 김광택;이준옥
    • 대한전자공학회논문지SD
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    • 제40권9호
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    • pp.651-657
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    • 2003
  • 얇은 중간 금속층을 가지는 측면 연마 광섬유 결합기를 이용한 편광분리기를 구현하였다. 실험 결과는 적절한 두께론 가지는 중간 금속층은 두 측면 연마된 광섬유 사이에서 TE 편광 성분의 광결합은 차단시키는 반면 TM 편광성분의 광결합은 허용함을 보여주었다. 측면 연마 광섬유를 이용한 편광분리기 설계 및 제작 기법을 기술하였다. 제작된 편광분리기는 TE와 TM 편광에 대하여 18dB와 23dB의 분리비를 보였다. 삽입손실은 TE 편광의 경우 0.7dB, TM 편광의 경우 1.3dB로 측정되었다.

얇은 금속 중간층이 포함된 광섬유-평면도파로 결합기 (Fiber-to-planar waveguide coupler with a thin metal intermediate layer)

  • 김광택;윤대성;손경락
    • 한국광학회지
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    • 제14권4호
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    • pp.355-358
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    • 2003
  • 얇은 금속 중간층이 있는 광섬유-평면도파로 결합기의 편광 및 파장 선택적 결합특성에 관한 실험 결과를 보고한다. 금속 박막층의 두께와 최상부층의 굴절률이 소자의 특성에 미치는 영향을 측정하고 그 결과를 설명하였다. 제안된 소자는 편광기, 광변조기 및 광센서 등의 다양한 응용 가능성을 보였다.

저온 동시소결을 위한 Ni-Zn-Cu 폐라이트와 Pb(Fe1/2Nb1/2)O3에서의 열적 거동 및 계면층 특성 (Interfacial Layer and Thermal Characteristics in Ni-Zn-Cu Ferrite and Pb(Fe1/2Nb1/2)O3 for the Low Temperature Co-sintering)

  • 송정환
    • 한국전기전자재료학회논문지
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    • 제20권10호
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    • pp.873-877
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    • 2007
  • In order to apply a complex multilayer chip LC filter, this study has estimated the interfacial reaction and coupling properties of dielectric materials $Pb(Fe_{1/2}Nb_{1/2})O_3$ and Ni-Zn-Cu ferrite materials through low-temperature co-sintering (LTCS). PFN powders were fabricated using double calcinated at $700^{\circ}C$ and then $850^{\circ}C$. While the perovskite phase rate was found to be 91 %, after heat treatment at $900^{\circ}C$ for 6h, the perovskite phase rate and density exhibited a value of 100 % and 7.46$g/cm^3$, respectively. The PFN/Ni-Zn-Cu ferrite, PFN/CUO (or $Pb_2Fe_2O_5$) and ferrite/CuO (or $Pb_2Fe_2O_5$) were mechanically coupled through interfacial reactions after the specimen was co-sintered at $900^{\circ}C$ for 6 h. No intermediate layer exists for the mutual coupling reaction. This result indicates the possibility of low-temperature co-sintering without any interfacial reaction layer for a multilayer chip LC filter.

Lattice Deformation and Electronic Structure of the $C_{60}{^+}$ Cation

  • 이기학;이한명;전희자;박성수;이왕로;Park, T. Y.;Xin Sun
    • Bulletin of the Korean Chemical Society
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    • 제17권5호
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    • pp.452-457
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    • 1996
  • The effects caused by the ionization on the electronic structure and geometry on C60 are studied by the modified Su-Schriffer-Heeger (SSH) model Hamiltonian. After the ionization of C60, the bond structure of the singly charged C60 cation is deformed from Ih symmetry of the neutral C60 to D5d, C1, and C2, which is dependent upon the change of the electron-phonon coupling strength. The electronic structure of the C60+ cation ground state undergoes Jahn-Teller distortion in the weak electron-phonon coupling region, while self-localized states occur in the intermediate electron-phonon region, but delocalized electronic states appear again in the strong electron-phonon region. In the realistic strength of the electron-phonon coupling in C60, the bond structure of C60+ shows the layer structure of the bond distortion and a polaron-like state is formed.

Magnetic Properties of Two-layered Ferromagnetic Films with a Conetic Intermediately Super-soft Magnetic Layer of Different Thickness

  • Choi, Jong-Gu;Sim, Jung-Taek;Kwak, Tae-Jun;Son, Il-Ho;Hwang, Do-Guwn;Rhee, Jang-Rho;Lee, Sang-Suk
    • 한국자기학회:학술대회 개요집
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    • 한국자기학회 2010년도 임시총회 및 하계학술연구발표회
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    • pp.148-150
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    • 2010
  • Two-layered ferromagnetic alloy films ($Ni_{80}Fe_{20}$, $Co_{90}Fe_{10}$) with a Conetic intermediate soft magnetic layer of different thickness were investigated to correlate the coercivity values and magnetization process with the strength of the hard saturation field. The interpretation of strong, medium and weak coupling is proposed.

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Overall Conversion Efficiency for Dimethylsulfide to Sulfur Dioxide in the Marine Boundary Layer-An Overview

  • Shon, Zang-Ho
    • Journal of Korean Society for Atmospheric Environment
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    • 제18권E2호
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    • pp.107-120
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    • 2002
  • Dimethyl sulfide (DMS) is the major sulfur gas released from the ocean. The atmospheric DMS released from the ocean is oxidized mainly by hydroxyl (OH) radical during the day and nitrate (NO$_3$) radical at night to form sulfur dioxide (SO$_2$) as well as other stable products. The oxidation mechanism of DMS via OH has been known to proceed by two channels; abstraction and addition channels. The major intermediate product of the addition channel has been known to be dimethylsulfoxide (DMSO) based on laboratory chamber studies and field experiments. However, a branching ratio for DMSO formation is still uncertain. The reaction of DMSO with OH ultimately produces SO$_2$and dimethylsulfone. The major product of the abstraction channel has known to be SO$_2$from laboratory chamber studies. But overall conversion efficiency for DMS to SO$_2$from DMS oxidation is still inconsistent in the literature. Based on laboratory and field studies, the conversion efficiency from the abstraction channel is likely to be greater than 0.5, while that from the addition channel is likely to be greater than 0.6. Overall conversion efficiency from DMS to SO$_2$might be greater than 0.5 based on the above two values in the remote marine boundary layer (MBL). This high efficiency in the remote MBL is supported by strong coupling between DMS and SO$_2$measurements with high temporal resolution.

Magnetic Properties of Nanocrystalline CoW Thin Film Alloys Electrodeposited from Citrate Baths

  • Park, Doek-Yong;Ko, Jang-Myoun
    • 전기화학회지
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    • 제6권4호
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    • pp.236-241
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    • 2003
  • Magnetic CoW thin film alloys were electrodeposited from citrate baths to investigate the resulting microstructure and magnetic properties. Deposit tungsten (W) content in the films electrodeposited at $70^{\circ}C$ were independent of current density, while coercivity decreased from hard $(H_{c,//}\~150\;Oe\;and\;H_{c.{\bot}}\;\~240\;Oe)$ to soft magnetic properties $(H_{c,//}\~20\;Oe\;and\;H_{c.{\bot}}\;\~30\;Oe)$ with increasing current densities from $10\;to\;100mA{\cdot}cm^2$, with deposit W content $(\~40\%)$ relatively unaffected by the applied current density. X-ray diffraction analysis indicated that hcp $Co_3W$ phases [(200), (201) and (220) planes] in the CoW films electrodeposited at $70^{\circ}C\;and\;10mA{\cdot}cm^{-2}$ were dominant, whereas amorphous CoW phases with small amount of hcp $Co_3W$ [(002) planes] were dominant with deposition at $70^{\circ}C\;and\;100mA{\cdot}cm^{-2}$. At intermediate current densities $(25\;and\;50mA{\cdot}cm^{-2}),\;hop\;Co_3W$ phases [(200), (002), (201) and (220)] were observed. The average grain size was measured to be 30 nm from Sheller formula. It is suggested that the change of the deposit coercivities in the CoW thin films electrodeposited at $70^{\circ}C$ is attributed to the change of microstructures with varying the current density. Nanostructured $Co_3W/amorphous-CoW$ multilayers were fabricated by alternating current density between 10 and $100 mA{\cdot}cm^{-2}$, varying the individual layer thickness. The magnetic properties of $Co_3W/amorphous-CoW$ multilayers were strongly dependent on the thickness of the alternating hard and soft magnetic thin films. The nanostructured $Co_3W/amorphous-CoW$ multilayers exhibited a shift from low to high coercivities suggesting a strong coupling effect.