• Journal of the Korean Vacuum Society
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• v.15 no.5
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• pp.493-498
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• 2006

Superluminescent diodes (SLD) with the emitting wavelength of $1.55{\mu}m$ was fabricated on InGaAs quantum dot structure grown by MOCVD. The output power and 3-dB bandwidth at room temperature and continuous wave operation were 3 mw and 55 nm, respectively.

• KIEE International Transactions on Electrophysics and Applications
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• v.5C no.1
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• pp.39-43
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• 2005

We proposed a structure for a 1.55 ㎛ strained separate confinement heterostructure (SCH) multi- quantum well (MQW) superluminescent diode (SLD), having a tapered active region. SLD was fabricated through a two-step procedure: the first step being metal organic chemical vapor deposition (MOCVD) and the second-step being liquid phase epitaxy (LPE). We used a 15 laterally tilted stripe and window region to suppress the lasing action of the SLD. The performance of the SLD showed output power of 11 mW with no lasing under 200 mA pulse driving. The full-width at half-maximum was 42 nm at 200 mA, 25℃.

• Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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• 2006.12a
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• pp.103-106
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• 2006

Semiconductor laser diode has a reflective facet in a both-ends side fundamentally. Laser performance for improving, Anti-Reflection and High-reflection coating on the facet of semiconductor laser diode. To prevent internal feedback from both facets for realizing superluminescent diode and reducing the reflection-induced intensity noise of laser diode, it's key techniques are AR/HR coatings. In the study AR coating film were manufactured by Ion-Assisted Deposition(IAD) system. Then manufactured coating film measurement electrical properties(L-I-V, Se, Resistor) and Optical properties (wavelength FFP)

• Proceedings of the Korean Institute of Information and Commucation Sciences Conference
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• 2003.05a
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• pp.370-373
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• 2003

Superluminescent diodes(SLDs) are the optimum light sources for application in optical measurement systems such as fiber gyroscopes, optical time domain reflectometers, and to short and medium distance optical communication systems. The broadband characteristics of SLDs reduce Rayleigh backscattering noise, polarization noise, and the bias offset due to the nonlinear Kerr effect in fiber gyro systems. In this paper, in order to suppress lasing oscillation, we introduced a laterally tilted SCH(Separate Confinement Heterostructure)-SLD with a window region. An output power of 11mW has been achieved at 200mA injection current at 25$^{\circ}C$. At 120mA, parallel and perpendicular to the junction were 31$^{\circ}$${\times}$38$^{\circ}$.

• Proceedings of the Korean Vacuum Society Conference
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• 2007.08a
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• pp.356-356
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• 2007

• Proceedings of the Optical Society of Korea Conference
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• 2000.02a
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• pp.282-283
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• 2000

본 연구에서는 사용한 양자 우물 구조는 그림 1과 같이 각 양자 우물의 두께가 다르게 분포되어 있다. 이러한 불균일 양자 우물 구조는 주로 광대역폭 반도체 광 증폭기를 위한 구조,$^{l).2)}$ 광대역폭 superluminescent diodes에 적용하기 위한 구조,$^{3)}$ 광대역폭 및 온도 비의존성 면발광 레이저를 위한 구조로 이용되고 있다.$^{4)}$ 이들 소자의 실현을 위해 우선 불균일 양자 우물 구조의 특성을 알아볼 필요가 있다. 따라서 본 연구에서는 이 구조를 CBE로 성장하고 릿지형 반도체 레이저를 제작하여 광학적 특성을 조사하였다. (중략)

• Journal of the Optical Society of Korea
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• v.17 no.2
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• pp.172-176
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• 2013

For demonstrating widely tunable external cavity lasers operating for near-infrared (NIR) wavelength, a flexible polymer waveguide with an imbedded Bragg grating is incorporated. Due to the superior flexibility of the polymer material, the reflection wavelength of the Bragg grating is widely tunable by imposing tensile and compressive strains on the flexible Bragg grating. A third-order Bragg grating is formed on the device for facilitating the fabrication method. With a superluminescent laser diode as a gain medium of ECL, the tunable laser exhibited output power of -3 dBm and a tuning range of 32 nm.

• Proceedings of the Korean Vacuum Society Conference
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• 2011.02a
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• pp.156-156
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• 2011

InAs와 InGaAs 양자점(Quantum Dot: QD)을 이용한 광대역 초발광 다이오드(Superluminescent Diode: SLD) 시료가 분자선증착법(Molecular Beam Epitaxy)을 이용하여 성장되었다. 광대역 파장대 출력을 얻기 위해 각기 다른 종류의 양자점과 다른 크기의 양자점을 적층하였다. 시료는 광발광(Photoluminescence: PL) 측정과 전계발광(Electroluminescence: EL) 측정을 통해 분석 되었으며, PL 측정결과 1222 nm와 1321 nm 파장에서 최대치(peak)를 나타냈으며 EL 측정결과 900mA 전류 주입시 131 nm의 반치폭(Full Width at Half Maximum: FWHM)을 얻었다.

• Applied Science and Convergence Technology
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• v.23 no.2
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• pp.97-102
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• 2014

A vacuum chamber for a commercial atomic force microscope (AFM) is designed and fabricated. Only minimal modifications were made to an existing microscope in an effort to work in a vacuum environment, while most of the available AFM functionalities were kept intact. The optical alignment needed for proper AFM operations including a SLD (superluminescent diode) and a photodiode can be made externally without breaking the vacuum. A vacuum level of $5{\times}10^{-3}$ torr was achieved with a mechanical pump. An enhancement of the quality factor was observed along with a shift in the resonance frequency of a non-contact-mode cantilever in a vacuum. Topographical data of a calibration sample were also obtained in air and in a low vacuum using the non-contact mode and the results were compared.

• Proceedings of the Optical Society of Korea Conference
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• 2000.08a
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• pp.32-33
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• 2000

최근 다른 두께로 조합된 양자 우물 구조를 이용한 연구가 다음과 같이 각각 다른 목적으로 진행되고 있다. 이러한 불균일 양자 우물 구조는 주로 광대역폭 반도체 광 증폭기를 위한 구조$^{l),2)}$ 광대역폭 Superluminescent Diode에 적용하기 위한 구조, $^{3)}$ 광대역폭 및 온도 비의존성 면발광 레이저를 위한 구조$^{4)}$ 로 이용되고 있으며 10여년 전에는 파장 조절 및 파장 스위칭을 위한 구조로 연구되었다.$^{5).6)}$ 이들 소자의 실현을 위해 우선 불균일 양자 우물 구조의 특성을 알아볼 필요가 있다. 본 연구에서 사용한 양자 우물 구조는 그림 1과 같이 각 양자 우물의 두께가 다르게 분포되어 있다. 그리고 이 구조를 CBE로 성장하고 릿지형 반도체 레이저를 제작하여 공진기 길이와 주입전류에 따른 발광 파장 특성으로부터 불균일 양자 우물 구조에서의 캐리어 분포 특성을 유추하였다. (중략)