• Optical Science and Technology
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• v.2 no.2
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• pp.44-51
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• 1998

광섬유 브래그 격자(fiber Bragg grating)는 광섬유 코어의 굴절율을 주기적으로 변조하여 특정 파장의 빛을 반사시키는 광섬유 소자로써 광섬유와의 연결 손실이 작고 파장 선택도가 높으며 편광에 무관한 특성 등으로 현재 전세계적으로 광통신용 소자나 광섬유 센서 등으로 활발히 연구되고 있다. 본 기술 해설에서는 이러한 광섬유 격자의 역사, 형성 원리 및 종류 등에 관해 알아보고, 단주기, 장주기 그리고 chirped 광섬유 격자의 특성에 대해 기술하였으며, 또한 광섬유 격자소자의 중요한 응용 분야인 광섬유 센서, 광섬유 레이저, 그리고 광통신에의 응용에 관해 소개하였다.

• Proceedings of the Optical Society of Korea Conference
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• 2001.02a
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• pp.192-193
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• 2001

높은 파장 선택도를 가지고 광신호를 제어하는 광섬유격자는 단주기 격자, 장주기 격자, 첩 격자 등이 있는데 이러한 격자의 제작 기술은 여러 응용분야에서 활용도 높은 소자를 제작하는 데 이용되어져 왔다. 본 논문에서는, 주어진 반사 파장 내에 매우 좁은 선폭의 여러 투과 스펙트럼 밴드를 가지며 그 응용성이 다양한 격자 제작을 목표로 이미 수행되어진 위상천이 격자의 시뮬레이션[1]을 토대로 $\pi$위상천이 격자를 제작하였다. (중략)

• Journal of the Korean Institute of Telematics and Electronics D
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• v.36D no.5
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• pp.80-87
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• 1999

We propose a new recirculating fiber delay-line filter structure. In proposed system, we insert a fiber Bragg grating(FBG) into a recirculating fiber delay line and it operates as a partially reflection mirror. Therefore, the transfer function of the system is given by the recirculating delay output part and the multiple-reflected output part due to a FBG. By adjusting the parameters such as coupling coefficient, reflectivity of FBG, and gain, we can make the system operate in various filter.

• Korean Journal of Optics and Photonics
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• v.15 no.4
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• pp.369-374
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• 2004

In this paper, we propose a new tunable laser diode structure. The laser diode consists of a sampled-grating distributed feedback laser diode monolithically integrated with a sampled-grating distributed-Brags-Reflector. For a specific design, the possibility of continuous/discrete wavelength tuning over 27nm is confirmed by a numerical analysis using a split-step time domain model. Because the laser diode can be directly coupled with optical fiber without the intervention of the passive section, the laser diode exhibits higher output power than the conventional laser diode.

• Proceedings of the Optical Society of Korea Conference
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• 2008.07a
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• pp.409-410
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• 2008

We have demonstrated a tunable Raman fiber laser using the combination of broadband CFBG and tunable fiber Bragg grating with the center wavelength 1415nm, which is tuned by adjusting longitudinal strain in the wavelength range from 1410 to 1420nm. A total output power of the tunable laser was about 0.9W with 13.8% of laser slope efficiency.

• Proceedings of the Optical Society of Korea Conference
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• 2003.07a
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• pp.214-215
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• 2003

평면광도파로 브래그격자는 광도파로 내부의 코어의 굴절률을 주기적으로 또는 비주기적으로 변화시켜 특정 파장의 빛을 반사시키거나 투과손실로 작용하게하는 광소자이다. 이러한 광소자는 광가감다중화기, 분산보상기, 파장선택형 반사거울, 파장제거필터, 증폭기의 이득평탄화, 광스위치등 여러분야의 소자 개발의 핵심적인 기능을 부여한다. UV 엑시머레이저의 출력을 게르마늄이 첨가된 실리카 유리에 조사하여 격자구조를 형성시키는 방법이 Hill 등에 의해 발표되었고 이후, 홀로그래피 방법, 위상마스크 방법등 여러 가지의 광섬유 격자 형성방법을 활용하여 여러종류의 광통신소자들이 연구되었다. (중략)

• Journal of the Korean Vacuum Society
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• v.15 no.3
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• pp.280-286
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• 2006

A distributed Bragg reflector (DBR) for the application of $1.3{\mu}m$ vertical cavity surface emitting laser (VCSEL) has grown by digital-alloy AlGaAs layer using the molecular beam epitaxy (MBE) method. The measured reflection spectra of the digital-alloy AlGaAs/GaAs DBR have uniformity in 0.35% over the 1/4 of 3-inch wafer. Furthermore, the TEM image showed that the composition and the thickness of the digital-alloy AlGaAs layer in AlGaAs/GaAs DBR was not affected by the temperature distribution over the wafer whole surface. Therefore, the digital-alloy AlGaAs/GaAs DBR can be used to get higher yield of VCSEL with the active medium of InAs quantum dots whose gain is inhomogeneously broadened.

• Journal of the Institute of Electronics Engineers of Korea SD
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• v.41 no.7
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• pp.31-36
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• 2004

In comparison with in-plane lasers, predicting the output power and differential quantum efficiency of Vertical-Cavity Surface-Emitting Lasers(VCSELs) is very difficult due to the distributed Bragg reflector(DBR) layers. Therefore, effective cavity model and transfer matrix method have been adapted in order to calculate the output power and differential quantum efficiency The effective cavity model is inappropriate to calculate output power and differential quantum efficiency while it is practically adequate to calculate the threshold gain and threshold current density The reason is that the effective cavity model can not take account of the absorption in GaAs stack layer right below the metal aperture. In this paper, we have compared the threshold current and differential quantum efficiency calculated by using transfer matrix method with effective cavity model and we have made a study of the validity of the effective cavity model. Finally, we have confirmed the versatility of the transfer matrix method with these studies.

• Korean Journal of Optics and Photonics
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• v.15 no.6
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• pp.591-596
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• 2004

In this paper, a photonic RF true-time delay based on a partially side-polished fiber Bragg grating with heating electrode has been proposed and fabricated. It features continuous voltage-controlled operation, requiring no mechanical perturbation and no moving parts. For an RF signal carried over an optical signal, the time delay has been obtained by controlling the voltage applied to the electrode and thus adjusting its reflection positions from the fiber grating via the thermooptic effect. The achieved time delay is about 100 ps with the electrical power consumption of 280 mW.

• Korean Journal of Optics and Photonics
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• v.9 no.2
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• pp.63-69
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• 1998

For detailed characterization of scattering losses occurring in VCSEL's distributed Bragg reflectors, we performed scattering experiment and obtained the information about surface roughness through the analysis of a modified transmission matrix method. The various wafers grown for VCSELs were used for the scattering experiment. The fractal surface assumption and extrapolation is used to estimate the scattered intensity near specular angle. The modified transmission matrix method employed in the analysis considers the scattering loss at each interface and calculates the reflectivity efficiently and easily. As a result, the surface roughness ranges from $4{\AA}$ to $10{\AA}$ The reduction of reflectivity due to the scattering amounts to 0.26% in case of $10{\AA}$ roughness.