• 제목/요약/키워드: InAs quantum dots

검색결과 276건 처리시간 0.02초

MEE법으로 성장한 InAs/GaAs 양자점의 발광특성 (Luminescence Properties of InAs/GaAs Quantum Dots Grown by MEE Method)

  • 오재원;변혜령;류미이;송진동
    • 한국진공학회지
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    • 제22권2호
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    • pp.92-97
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    • 2013
  • Migration-enhanced epitaxy 성장한 InAs/GaAs 양자점(quantum dots)의 광학적 특성을 PL (photoluminescence)과 Time-resolved PL 이용하여 분석하였다. InAs 양자점은 In을 9.3초 공급하고 5초 차단한 후 As을 3초, 4초, 6초, 또는 9초 공급하고 5초 차단하는 과정을 3회 반복하여 성장하였다. As을 3초 공급한 시료의 PL 피크는 1,140 nm에서 나타나고, PL 세기는 다른 세 시료에 비해 매우 약하게 나타났다. As 공급시간을 3초에서 증가하였을 때 모든 PL 피크는 1,118 nm로 청색이동하여 나타났으며, PL 세기는 증가하였다. As을 6초 공급한 시료의 PL 세기가 가장 강하게 나타나고, 반치폭(full width at half maximum)도 가장 좁게 나타났다. 이러한 결과는 양자점의 밀도와 균일도(크기변화)로 설명된다. 또한 발광파장에 따른 PL 소멸시간은 PL 피크 근처에서 가장 길게 나타났다.

P 변조도핑한 In(Ga)As/InGaAsP 양자점에 대한 운반자 동역학 (Carrier Dynamics of P-modulation Doped In(Ga)A/InGaAsP Quantum Dots)

  • 장유동;박재규;이동한;홍성의;오대곤
    • 한국진공학회지
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    • 제15권3호
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    • pp.301-307
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    • 2006
  • P-modulation doping된 In(Ga)As/InGaAsP 양자점에서의 decay time 특성을 undoped 양자점 시료와의 비교를 통해 살펴보았다. 10 K 에서의 photoluminescence (PL) 세기는 doping 된 양자점이 doping되지 않은 양자점에 비해 약 10배 정도 약하게 나왔다. 또한 Time resolved PL (TR-PL) 실험을 통해 얻은 양자점 시료의 기저상태 PL peak 에서의 decay time은 doping된 양자점이 doping 되지 않은 양자점에 비해 매우 짧게 나왔다. 이러한 PL 세기와 decay time 특성을 통해서 본 연구에서 측정한 doping 된 양자점의 경우에는 doping에 의해 결함이 증가하게 되고, 그로 인해 운반자의 비발광 경로가 증가하게 되어 doping 된 양자점의 경우에 decay time이 짧게 나타나는 것으로 분석하였다.

광화학적 방법을 통한 InP계 양자점 표면결함 부동태화 연구 (Study on Surface-defect Passivation of InP System Quantum Dots by Photochemical Method)

  • 김도연;박현수;조혜미;김범성;김우병
    • 한국분말재료학회지
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    • 제24권6호
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    • pp.489-493
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    • 2017
  • In this study, the surface passivation process for InP-based quantum dots (QDs) is investigated. Surface coating is performed with poly(methylmethacrylate) (PMMA) and thioglycolic acid. The quantum yield (QY) of a PMMA-coated sample slightly increases by approximately 1.3% relative to that of the as-synthesized InP/ZnS QDs. The QYs of the uncoated and PMMA-coated samples drastically decrease after 16 days because of the high defect state density of the InP-based QDs. PMMA does not have a significant effect on the defect passivation. Thioglycolic acid is investigated in this study for the effective surface passivation of InP-based QDs. Surface passivation with thioglycolic acid is more effective than that with the PMMA coating, and the QY increases from 1.7% to 11.3%. ZnS formed on the surface of the InP QDs and S in thioglycolic acid show strong bonding property. Additionally, the QY is further increased up to 21.0% by the photochemical reaction. Electron-hole pairs are formed by light irradiation and lead to strong bonding between the inorganic and thioglycolic acid sulfur. The surface of the InP core QDs, which does not emit light, is passivated by the irradiated light and emits green light after the photochemical reaction.

Syntheses of CdTe Quantum Dots and Nanoparticles through Simple Sonochemical Method under Multibubble Sonoluminescence Conditions

  • Hwang, Cha-Hwan;Park, Jong-Pil;Song, Mi-Yeon;Lee, Jin-Ho;Shim, Il-Wun
    • Bulletin of the Korean Chemical Society
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    • 제32권7호
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    • pp.2207-2211
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    • 2011
  • Colloidal cadmium telluride (CdTe) quantum dots (QDs) and their nanoparticles have been synthesized by one pot sonochemical reactions under multibubble sonoluminescence (MBSL) conditions, which are quite mild and facile compared to other typical high temperature solution-based methods. For a typical reaction, $CdCl_2$ and tellurium powder with hexadecylamine and trioctylphosphine/trioctylphosphineoxide (TOP/TOPO) as a dispersant were sonicated in toluene solvent at 20 KHz and a power of 220W for 5-40 min at 60 $^{\circ}C$. The sizes of CdTe particles, in a very wide size range from 2 nm-30 ${\mu}m$, were controllable by varying the sonicating and thermal heating conditions. The prepared CdTe QDs show different colors from pale yellow to dark brown and corresponding photoluminescence properties due mainly to the quantum confinement effect. The CdTe nanoparticles of about 20 nm in average were found to have band gap of 1.53 eV, which is the most optimally matched band gap to solar spectrum.

Electrochemical Biosensors based on Nanocomposites of Carbon-based Dots

  • Ngo, Yen-Linh Thi;Jana, Jayasmita;Chung, Jin Suk;Hur, Seung Hyun
    • Korean Chemical Engineering Research
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    • 제58권4호
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    • pp.499-513
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    • 2020
  • Among the many studies of carbon-based nanomaterials, carbon-based dots (CDs) have attracted considerable interest owing to their large surface area, intrinsic low-toxicity, excellent biocompatibility, high solubility, and low-cost with environmentally friendly routes, as well as their ability for modification with other nanomaterials. CDs have several applications in biosensing, photocatalysis, bioimaging, and nanomedicine. In addition, the fascinating electrochemical properties of CDs, including high active surface area, excellent electrical conductivity, electrocatalytic activity, high porosity, and adsorption capability, make them potential candidates for electrochemical sensing materials. This paper reviews the recent developments and synthesis of CDs and their composites for the proposed electrochemical sensing platforms. The electrochemical principles and future perspective and challenges of electrochemical biosensors are also discussed based on CDs-nanocomposites.

TEM Study on the Growth Characteristics of Self-Assembled InAs/GaAs Quantum Dots

  • Kim, Hyung-Seok;Suh, Ju-Hyung;Park, Chan-Gyung;Lee, Sang-Jun;Noh, Sam-Gyu;Song, Jin-Dong;Park, Yong-Ju;Lee, Jung-Il
    • Applied Microscopy
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    • 제36권spc1호
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    • pp.35-40
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    • 2006
  • Self-assembled InAs/GaAs quantum dots (QDs) were grown by the atomic layer epitaxy (ALE) and molecular beam epitaxy (MBE) techniques, The structure and the thermal stability of QDs have been studied by high resolution electron microscopy with in-situ heating experiment capability, The ALE and MBE QDs were found to form a hemispherical structure with side facets in the early stage of growth, Upon capping by GaAs layer, however, the apex of QDs changed to a flat one. The ALE QDs have larger size and more regular shape than those of MBE QDs. The QDs collapse due to elevated temperature was observed directly in atomic scale, In situ heating experiment within TEM revealed that the uncapped QDs remained stable up to $580^{\circ}C$, However, at temperature above $600^{\circ}C$, the QDs collapsed due to the diffusion and evaporation of In and As from the QDs, The density of the QDs decreased abruptly by this collapse and most of them disappeared at above $600^{\circ}C$.

Enhancement of the surface plasmon-polariton excitation in nanometer metal films

  • Kukushkin, Vladimir A.;Baidus, Nikoly V.
    • Advances in nano research
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    • 제2권3호
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    • pp.173-177
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    • 2014
  • This study is aimed to the numerical modeling of the surface plasmon-polariton excitation by a layer of active (electrically pumped) quantum dots embedded in a semiconductor, covered with a metal. It is shown that this excitation becomes much more efficient if the metal has a form of a thin (with thickness of several nanometers) film. The cause of this enhancement in comparison with a thick covering metal film is the partial surface plasmon-polariton localized at the metal-semiconductor interface penetration into air. In result the real part of the metal+air half-space effective dielectric function becomes closer (in absolute value) to the real part of the semiconductor dielectric function than in the case of a thick covering metal film. This leads to approaching the point of the surface plasmon-polariton resonance (where absolute values of these parts coincide) and, therefore, the enhancement of the surface plasmon-polariton excitation. The calculations were made for a particular example of InAs quantum dot layer embedded in GaAs matrix covered with an Au film. Its results indicate that for the 10 nm Au film the rate of this excitation becomes by 2.5 times, and for the 5 nm Au film - by 6-7 times larger than in the case of a thick (40 nm or more) Au film.

Controlling Quantum Confinement and Magnetic Doping of Cesium Lead Halide Perovskite Nanocrystals

  • Dong, Yitong;Parobek, David;Son, Dong Hee
    • 한국세라믹학회지
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    • 제55권6호
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    • pp.515-526
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    • 2018
  • Cesium lead halide ($CsPbX_3$) nanocrystals have emerged as a new family of semiconductor nanomaterials that can outperform existing semiconductor nanocrystals owing to their superb optical and charge transport properties. Although these materials are expected to have many superior properties, control of the quantum confinement and isoelectronic magnetic doping, which can greatly enhance their optical, electronic, and magnetic properties, has faced significant challenges. These obstacles have hindered full utilization of the benefits that can be obtained by using $CsPbX_3$ nanocrystals exhibiting strong quantum confinement or coupling between exciton and magnetic dopants, which have been extensively explored in many other semiconductor quantum dots. Here, we review progress made during the past several years in tackling the issues of introducing controllable quantum confinement and doping of $Mn^{2+}$ ions as the prototypical magnetic dopant in colloidal $CsPbX_3$ nanocrystals.

Growth features and nucleation mechanism of Ga1-x-yInxAlyN material system on GaN substrate

  • Simonyan, Arpine K.;Gambaryan, Karen M.;Aroutiounian, Vladimir M.
    • Advances in nano research
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    • 제5권4호
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    • pp.303-311
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    • 2017
  • The continuum elasticity model is applied to investigate quantitatively the growth features and nucleation mechanism of quantum dots, nanopits, and joint QDs-nanopits structures in GaInAlN quasyternary systems. We have shown that for GaInAlN material system at the critical strain of ${\varepsilon}^*=0.039$ the sign of critical energy and volume is changed. We assume that at ${\varepsilon}={\varepsilon}^*$ the mechanism of the nucleation is changed from the growth of quantum dots to the nucleation of nanopits. Obviously, at small misfit (${\varepsilon}$ < ${\varepsilon}^*$), the bulk nucleation mechanism dominates. However, at ${\varepsilon}$ > ${\varepsilon}^*$, when the energy barrier becomes negative as well as a larger misfit provides a low-barrier path for the formation of dislocations, the nucleation of pits becomes energetically preferable. The free energy of mixing for $Ga_{1-x-y}In_xAl_yN$ quasiternary system was calculated and studied and its 3D sketch was plotted.

Direct Comparison of Optical Properties from Graphene Oxide Quantum Dots and Graphene Oxide

  • Jang, Min-Ho;Ha, Hyun Dong;Seo, Tae Seok;Cho, Yong-Hoon
    • Applied Science and Convergence Technology
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    • 제24권4호
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    • pp.111-116
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    • 2015
  • The graphene oxide (GO) and graphene oxide quantum dots (GOQDs), which have gained research interest as new types of light-emitting materials, were synthesized by the modified Hummers method for oxidation of graphite flake and graphite nanoparticle. The optical properties of GO and GOQDs have been compared by mean of photoluminescence (PL), PL excitation (PLE), UV-vis absorbance, and time-resolved PL. The GO have an absorption peak at 229 nm and shoulder part at 310 nm, whereas the GOQDs show broad absorption with a gradual change up without any absorption peaks. The PL emission of GOQDs and GO showed the green color at 520 nm and the red color at 690 nm, respectively. The red emission of GO showed faster PL decay time than the green emission of GOQDs. In particular, the temporal PL profile of the GO showed redshift from 560 nm to 660 nm after the pump event.