• Proceedings of the Korean Institute of Communication Sciences Conference
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• 2006.07a
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• pp.386-386
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• 2006

• Proceedings of the KIEE Conference
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• 1999.11d
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• pp.1126-1127
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• 1999

연산자 분리 시영역 모델을 이용하여 광섬유 커플러 ADM(add-drop multiplexer)의 필터링 효과를 분석하였다. 이 모델은 방향성 결합기나 브래그 격자를 포함하는 소자의 해석에 유용하다. 본 논문에서는 비대칭 구조를 고려했으며 결합계수, 코어의 반경, 개구수, 굴절율 변조 등의 파라미터를 이용하여 최적의 필터링 효과를 얻기 위한 구조를 설계하였다.

• Proceedings of the Optical Society of Korea Conference
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• 2003.02a
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• pp.174-175
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• 2003

광섬유-평면도파로 결합기는 평면도파로의 재료와 구조에 따라 다양한 응응이 가능하다. 특히 평면도파로의 전기광학 효과를 이용하면 고속 광변조 현상을 얻을 수 있다. 평면도파롱에 전기장을 인가하기 위해서는 두개의 도체 전극이 필요하다. 전극으로 주로 금속을 많이 이용하기 때문에 금속층이 포함된 광섬유-평면도파로 결합기의 특성을 연구하는 것이 요구된다. 본 논문에서 그림 1과 같이 금속 중간층이 포함된 광섬유-평면도파로 결합기의 구조의 동작특성을 측정하고 결과를 보고한다. (중략)

• Proceedings of the Optical Society of Korea Conference
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• 2001.02a
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• pp.216-217
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• 2001

광섬유와 평면 도파로를 결합한 도파로 구조에서 광 결합 현상은 다양한 응용 가능성 때문에 이론적으로 또는 실험적으로 많은 연구가 되어오고 있다. 광섬유는 단일모드를 이용하고 적당한 곡률이 주어진 블록에 고정한 후 연마하여 클래딩의 일부를 제거하고, 그 상부에 다중모드 평면 도파로(Multi-Mode Overlay Waveguide; MMOW)를 구성한다. 제작된 결합기 구조에서 평면 도파로는 광섬유의 감쇠장 결합(Evanescent field coupling)을 유도하게 되므로, 소자의 특성은 평면 도파로의 구조와 조건에 의해 결정된다. (중략)

• Proceedings of the Optical Society of Korea Conference
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• 2000.08a
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• pp.138-139
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• 2000

광섬유-평면도파로 결합기는 측면 연마된 광섬유와 그 위에 올려진 평면도파로 사이의 소산장 결합(evanescent field coupling)를 이용하는 소자이다. 이 결합기는 기본적으로 파장선택성과 편광선택성을 있고, 삽입손실이 매우 작고 기계적 신뢰성이 우수하여 많은 주목을 받아 왔다. 평면도파로의 재료로 반도체, 크리스탈, 액정크리스탈, 폴리머등 다양한 물질이 이용될 수 있어 광통신뿐만 아니라 광 센서 분야에서 활발하게 연구되어 왔다. (중략)

• Proceedings of the Optical Society of Korea Conference
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• 2003.07a
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• pp.18-19
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• 2003

측면 연마 광섬유 결합기는 비록 제작 공정이 다소 복잡하지만 다양한 응용이 가능하기 때문에 많은 연구가 진행 되어 왔다. 특히 최근에는 광센서나 초고속 광통신망에 편광 유지 광섬유를 이용한 광학소자의 필요성이 증가 하고 있다. 본 논문은 얇은 중간 금속 층을 가지는 측면 연마 편광 유지 광섬유 결합기를 이용한 편광 분리기에 관한 실험 연구 결과를 보고한다. (중략)

• Korean Journal of Optics and Photonics
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• v.10 no.5
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• pp.419-423
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• 1999

Optical filters utilizing the evanescent filed coupling between the side polished fiber and polymer planar waveguide were fabricated and optical properties of the devices were measured. A scheme for reducing polarization dependent properties of the device was proposed and demonstrated experimentally. Our measurement results showed that resonance wavelengths and filtering depth of the optical filters can be determined by adjusting thickness of planar waveguide and polishing depth of the fiber. The device fabrication procedure including fiber polishing steps and formation of polymer planar waveguide were described. The optical characteristics of fabricated optical filers were that 3 dB bandwidth was 15 nm, the resonance wavelength difference between the TE and TM polarized response was less then 2 nm, and insertion loss was less then 0.2 dB. The measured resonance wavelength drift dut to the variation of ambient temperature was -0.35 nm/$^{\circ}C$.

• Transactions of the Korean Society for Noise and Vibration Engineering
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• v.22 no.7
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• pp.626-633
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• 2012

In this paper, sound pressure sensitivity of the fiber optic acoustic sensor according to sensor direction and mandrel material were investigated experimentally. Three different directions were selected as stand, lay, and hole. Hollow cylinder type mandrel dimension is 30 mm in outer diameter, 45 mm in length, and 2 mm in thickness, and about 50 m optical fibers were wounded on the surface of the mandrel. Non-directional sound speaker was used as a sound source. Sagnac interferometer and single mode fiber, a laser with 1,550 nm in wavelength, $2{\times}2$ coupler were used. Based on the experimental results, lay direction's sensitivity is the highest in the frequency range of 2 kHz~4 kHz. 'PTFE+carbon' material is more sensitive than PTFE in the frequency range of 5 kHz~20 kHz. Sound pressure detection sensitivity depends on the mandrel direction and material under certain frequency.

• Korean Journal of Optics and Photonics
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• v.31 no.5
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• pp.213-217
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• 2020

In this study we report a wet-etching-based fabrication method for adiabatic optical-fiber tapers (OFTs), and describe their adiabaticity and HE₁₁ mode evolution at a wavelength of 1550 nm. The profile of the fabricated system satisfies the adiabaticity properties well, and the far-field pattern from the etched OFT shows that the fundamental HE₁₁ mode is maintained without a higher-order mode coupling throughout the tapers. In addition, the measured far-field pattern agrees well with the simulated result. The proposed adiabatic OFTs can be applied to a number of photonic applications, especially fiber-chip packages. Based on the fabricated adiabatic OFT structures, the optical transmission to the inversely tapered silicon waveguide shows large spatial-dimensional tolerances for 1 dB excess loss of ~60 ㎛ (silicon waveguide angle of 1°) and insertion loss of less than 0.4 dB (silicon waveguide angle of 4°), from the numerical simulation. The proposed adiabatic coupler shows the ultrabroadband coupling efficiency over the O- and C-bands.

• The Journal of Korean Institute of Communications and Information Sciences
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• v.18 no.9
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• pp.1248-1256
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• 1993

The propagation and delay properties in opical fiber are particularly attractive because digital signal processing and conventional analog signal processing techniques such as those using surface acoustic wave devices are limited In their usefulness for signal bandwidth exceeding one or two GHz, although they are very effective at lower frequencies. Since an accurate, low loss and short time delay elements can be obtained by using such an optical fiber, optical signal precessing has attracted much attention for high speed and broad-band signal precessing in particular channel separation filtering for optical FDM signals. In this paper, we consider a coherent optical lattice filter, which uses coherent light sources and consists of directional couplers and optical fiber delay elemnts. The optical fiber fitters are more restricted than the usual digital filters. The reasons are as follows. 1) the coupling coefficients of directional couplers are restricted to the number between 0 and 1. 2) optical signal E(complex amplitude) is divided into J If-$\boxUl$ and J L/7$\div$$\boxUl$ at the directional coupler. Considering these restrictions and in this case all the coupling coefficients of summing and branching elements are set to be equal, we have given design formulae for optical lattice filter, which make the best use of optical signal energy.