• Title/Summary/Keyword: MQW

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Generation of Coherent LO Phonons in GaAs/AlGaAs MQW's by the Impulsive Stimulated Raman Scattering (GaAs/AlGaAs 양자우물 구조에서 Impulsive Stimulated Raman Scattering 방법에 의한 결맞는 포논의 생성)

  • 이기주;이대수;조영달;임용식;김대식
    • Proceedings of the Optical Society of Korea Conference
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    • 2000.02a
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    • pp.24-25
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    • 2000
  • After the invention of the femtosecond pulse lasers, generating and detecting the coherent optical phonons in various materials became possible. In bulk GaAs, which is a polar material, the coherent LO phonons are known to be generated by the ultrafast screening of the surface space-charge fields. However, little is known about the generation mechanisms of coherent phonons in GaAs quantum structures. (omitted)

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Lasing Characteristics of MQW Waveguide-type Depleted Optical Thristor Operating at 1.561um (1.561um에서 동작하는 MQW 도파로형 Depleted Optical Thyristor의 레이징 특성 분석)

  • Choi Woon Kyung;Kim Doo-Gun;Choi Young-Wan;Lee Seok;Woo Deok-Ha;Kim Sun-Ho
    • Journal of the Institute of Electronics Engineers of Korea SD
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    • v.41 no.1
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    • pp.29-34
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    • 2004
  • We present the first demonstration of waveguide-type depleted optical thyristor laser diode with InGaAs/InGaAsP multiple quantum well structure. The measured switching voltage and current are 4.63 V and 10uA respectively. The holding voltage and current are respectively 0.59 V, 20uA. The lasing threshold current at the temperature of $25^{\circ}C$ and $10^{\circ}C$ are 111 mAA and 72.5 mA, respectively. The lasing wavelength is centered at 1.561um at a bias current equal to 1.41 times threshold.

Time-resolved photoluminescence spectroscopy of InGaN multiple quantum wells

  • Lee, Joo-In;Shin, Eun-joo;Lee, J.Y. m;Kim, S.T.;G.S. Lim;Lee, H.G.
    • Journal of Korean Vacuum Science & Technology
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    • v.4 no.1
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    • pp.23-26
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    • 2000
  • We have fabricated by metal organic chemical vapor deposition (MOCVD) In$\_$0.13/Ga$\_$0.87/N/GaN multiple quantum well (MQW) with thickness as thin as 10 A and barriers also of th same width on (0001) sapphire substrate. We have investigated this thin MQW by steady-state and time-resolved photoluminescence(PL) in picosecond time scale in a wide temperature range from 10 to 290 K. In the PL at 10 K, we observed a broad peak at 3.134 eV which was attributed to the quantum well emission of InGaN. The full width at half maximum (FWHM) of this peak was 129 meV at 10 K and its broadening at low temperatures was considered to be due to compositional fluctuations and interfacial disorder in the alloy. The narrow width of the quantum well was mainly responsible for the broadening of the emission linewidth. We also observed an intense and sharp peak at 3.471 eV of GaN barrier. From the temperature dependent PL measurements, the activation energy of the InGaN quantum well emision peak was estimated to be 69 meV. The lifetime of the quantum well emission was found to be 720 ps at 10 K, which was explained in terms of the exciton localization arising from potential fluctuations.

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Terahertz Detection Characteristics of Low-Temperature Grown InGaAs/InAlAs Multi Quantum Well

  • Park, Dong-U;Han, Im-Sik;Kim, Chang-Su;No, Sam-Gyu;Ji, Yeong-Bin;Tae, In;Lee, Gi-Ju;Kim, Jin-Su;Kim, Jong-Su
    • Proceedings of the Korean Vacuum Society Conference
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    • 2013.02a
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    • pp.317-318
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    • 2013
  • Terahertz (THz) wave는 광학 영역과 방송파 영역 사이에 광대역 주파수 스펙트럼을 차지하고 있다. X선과는 달리 비이온화 광원으로 직진성, 투과성, 낮은 에너지 (meV)를 가지고 있어 비파괴적이고 무해한 장점을 지니고 있다. 본 연구에서는 In0.53Ga0.47As:Be/In0.52Al0.48As의 multi quantum well (MQW)을 Semi-insulting InP:Fe substrate 위에 active layer의 두께와 적층을 변화주어서 성장하였고Au (200 nm)/Ti (30 nm)의 금속전극으로 공정을 하였다. Ti:Sapphire femtosecond pulse laser를 조사하여 THz time-domain spectrometer 시스템을 이용하여 광전도검출법으로 THz 검출 특성을 연구하였다. THz 검출은 짧은 전하수명과 높은 저항을 요구한다. LTInGaAs의 경우 AsGa antisite로 인하여 짧은 전하수명을 얻게 되면 n-type의 높은 전하밀도를 가지게 되어서 저항이 낮아지게 된다. 높은 저항을 만들기 위하여 Be doping을 이용하여 과잉의 전자들을 보상하고 InAlAs layer를 삽입시켜 보다 높은 저항을 얻었다. LT-InGaAs:Be는 LT-GaAs보다 1/70 정도의 amplitude를 보이는데 LT-InGaAs/InAlAs MQW의 경우 LT-GaAs 대비 약 3/4 정도의 큰 amplitude를 얻었다. 또 active layer의 두께가 얇고 적층이 많을수록 신호가 커지는 것을 알 수 있었다. 이는 상대적으로 band gap이 큰 InAlAs층이 더 높은 저항을 만든 것으로 사료된다.

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Development of GaInP-AlGaInP High Power Red Laser Diodes

  • Kim, Ho-Gyeong;Kim, Chang-Ju;Choe, Jae-Hyeok;Bae, Seong-Ju;Song, Geun-Man;Sin, Chan-Su;Go, Cheol-Gi
    • Proceedings of the Korean Vacuum Society Conference
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    • 2013.02a
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    • pp.118-119
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    • 2013
  • High power, short wavelength red laser diodes (LDs) have attracted significant interests in a variety of fields due to their advantages in terms of reliability, compactness and cost. The higher brightness for human eyes is required, the shorter wavelength like 630 nm is necessary with higher output power. In this respect, LDs are promising as alternative candidates of gas or dye lasers for such applications due to their small size, high optical/electrical power conversion efficiency, robustness and so on. The crystalline quality of GaInP-AlGaInP multiple quantum wells (MQWs) and AlInP cladding layers is a crucial part in the device performance of GaInP red LDs. Here, we first investigated the effect of Si diffusion on the optical properties of GaInP-AlGaInP MQWs grown with different growth temperatures. Secondary ion mass spectroscopy (SIMS) measurements revealed that both the Mg and Si diffusion into MQW active region was significant. To reduce such diffusion, we employed undoped Mg and Si diffusion barrier and could improve the properties.Without both Mg and Si diffusion barriers, no lasing emission was observed. However, lasing emission was observed clearly for the red LDs with both Mg and Si diffusion barriers. We then investigated the temperature dependent optical properties of MQW layers grown with different well thicknesses (6, 8 and 10 nm). When the well thickness was 10 nm, the better crystalline quality was obtained. However, the observed LD performances were similar, probably due to the defects and impurities in the AlGaInP layer. Further investigation with the detailed analyses will be presented later.

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SPICE Simulation of All-Optical Transmitter/Receiver Circuits Configured with MQW Optical Modulators and FETs (다층 양자우물구조 광 변조기와 전계효과 트랜지스터를 사용한 광 송/수신기회로의 SPICE 모사)

  • 이유종
    • Proceedings of the Korean Institute of Information and Commucation Sciences Conference
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    • 1999.05a
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    • pp.420-424
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    • 1999
  • In this paper, an optical switching circuit and several types of all-optical transmitter/receiver circuits which are configured with photodiodes, multiple quantum-well(MQW) optical modulators, and field-effect transistors(FETs) were simulated using PSPICE and their results of these are examined and discussed. 20 $\mu\textrm{m}$ ${\times}$ 20 $\mu\textrm{m}$ of window size was used for the optical modulators and 100 $\mu\textrm{m}$ wide FETs with the transconductance value of 55 mS/mm were used for the simulations. Simulation results clearly show that in order for the high speed operation of the all-optical circuits, the size of each device should be minimized to reduce the parasitic capacitance, the circuits should be designed to operate at the wavelength where the resposivity of photodiodes becomes the maximum peak, and the use of short, high-intensity input optical signal beams is very advantageous.

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1.31 um Uncooled DFB-LD with High Slope Efficiency for G-PON Application (G-PON용 높은 전광변환효율을 갖는 1.31 um 비냉각 DFB-LD)

  • Kim, Jeong-Ho;Pi, Joong-Ho;Kim, Deok-Hyun;Park, Chil-Sung;Ryu, Han-Gwon;Koo, Bon-Jo
    • Korean Journal of Optics and Photonics
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    • v.18 no.5
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    • pp.333-336
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    • 2007
  • A Strained Layer Multiquantum-Well (SL-MQW) distributed feedback laser at a wavelength of 1.31 um operating from $-40^{\circ}C$ to $85^{\circ}C$ without any cooling is grown by metal-organic chemical vapor deposition (MOCVD). Lasers with high slope efficiency are achieved through careful optimization of a SL-MQW active layer, especiallyoptimizing the amount of strain, the well thickness, the barrier thickness, the number of wells, and the active layer width. In this paper, we obtain the slope efficiencies of 0.38[mW/mA] and 0.26 [mW/mA] at $25^{\circ}C$ and $85^{\circ}C$, respectively. Threshold currents are 7.1[mA] and 19.8[mA] at $25^{\circ}C$ and $85^{\circ}C$, respectively.