• Title/Summary/Keyword: InAs quantum dot

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The Simulation of Si quantum Dot Formation in PVD Process (PVD 공정을 이용한 Si 양자점 형성 전산모사)

  • Kim, Yun-Sung;Chung, Yong-Chae
    • Journal of the Korean Ceramic Society
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    • v.39 no.5
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    • pp.517-522
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    • 2002
  • In this study, the effect of the processing parameters in PVD process on the size and the distribution of deposited Si quantum dots was quantitatively investigated by computational simulation utilizing Monte Carlo method. The processing parameters, substrate temperature, deposition time, gas pressure and target-substrate distance were selected as variables since those parameters are often selected as variables in PVD experiments. It is predicted that the density of $1{\times}10^{12}cm^{-2}$ Si quantum dots can be deposited on the substrate when the deposition rate is 0.05 nm/sec at the substrate temperature of 490${\circ}$, deposition time of 7 sec, gas pressure of 3 mTorr and target-substrate distance of 8 cm.

Temperature Dependent Photoluminescence from InAs/GaAs Quantum Dots Grown by Molecular Beam Epitaxy

  • Lee, Kyoung Su;Oh, Gyujin;Kim, Eun Kyu;Song, Jin Dong
    • Applied Science and Convergence Technology
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    • v.26 no.4
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    • pp.86-90
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    • 2017
  • We have reported structural and optical properties of self-assembled InAs/GaAs quantum dot (QD) grown by molecular beam epitaxy with different arsenic to indium flux ratios (V/III ratios). By increasing the V/III ratio from 9 to 160, average diameter and height of the InAs QDs decreased, but areal density of them increased. The InAs QDs grown under V/III ratio of 30 had a highest-aspect-ratio of 0.134 among them grown with other conditions. Optical property of the InAs QD was investigated by the temperature-dependent photoluminescence (PL) and integrated PL. From the temperature dependence PL measurements of InAs QDs, the activation energies of $E_{a1}$ and $E_{a2}$ for the InAs QDs were obtained $48{\pm}3meV$ and $229{\pm}23meV$, respectively. It was considered that the values of $E_{a1}$ and $E_{a2}$ are corresponded to the energy difference between ground-state and first excited state, and the energy difference between ground-state and wetting layer, respectively.

Design of QCA Content-Addressable Memory Cell for Quantum Computer Environment (양자컴퓨터 환경에서의 QCA 기반 내용주소화 메모리 셀 설계)

  • Park, Chae-Seong;Jeon, Jun-Cheol
    • The Journal of the Convergence on Culture Technology
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    • v.6 no.2
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    • pp.521-527
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    • 2020
  • Quantum-dot cellular automata (QCA) is a technology that attracts attention as a next-generation digital circuit design technology, and several digital circuits have been proposed in the QCA environment. Content-addressable memory (CAM) is a storage device that conducts a search based on information stored therein and provides fast speed in a special process such as network switching. Existing CAM cell circuits proposed in the QCA environment have a disadvantage in that a required area and energy dissipation are large. The CAM cell is composed of a memory unit that stores information and a match unit that determines whether or not the search is successful, and this study proposes an improved QCA CAM cell by designing the memory unit in a multi-layer structure. The proposed circuit uses simulation to verify the operation and compares and analyzes with the existing circuit.

Multilayer QCA D-latch design using cell interaction (셀 간 상호작용을 이용한 다층구조 QCA D-래치 설계)

  • Jang, Woo-Yeong;Jeon, Jun-Cheol
    • The Journal of the Convergence on Culture Technology
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    • v.6 no.2
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    • pp.515-520
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    • 2020
  • CMOS used in digital circuit design technology has reached the limit of integration due to quantum tunneling. Quantum-dot cellular automata (QCA), which can replace this, has many advantages such as low power consumption and fast switching speed, so many digital circuits of CMOS have been proposed based on QCA. Among them, the multiplexer is a basic circuit used in various circuits such as D-flip-flops and resistors, and has been studied a lot. However, the existing multiplexer has a disadvantage that space efficiency is not good. Therefore, in this paper, we propose a new multilayered multiplexer using cell interaction and D-latch using it. The multiplexer and D-latch proposed in this paper have improved area, cell count, and delay time, and have excellent connectivity and scalability when designing large circuits. All proposed structures are simulated using QCADesigner to verify operation.

Study of Light-induced Degradation in Thin Film Silicon Solar Cells: Hydrogenated Amorphous Silicon Solar Cell and Nano-quantum Dot Silicon Thin Film Solar Cell (박막 실리콘 태양전지의 광열화현상 연구: 비정질 실리콘 태양전지 및 나노양자점 실리콘 박막 태양전지)

  • Kim, Ka-Hyun
    • Journal of the Korean Solar Energy Society
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    • v.39 no.1
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    • pp.1-9
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    • 2019
  • Light induced degradation is one of the major research challenges of hydrogenated amorphous silicon related thin film silicon solar cells. Amorphous silicon shows creation of metastable defect states, originating from elevated concentration of dangling bonds during light exposure. The metastable defect states work as recombination centers, and mostly affects quality of intrinsic layer in solar cells. In this paper we present results of light induced degradation in thin film silicon solar cells and discussion on physical origin, mechanism and practical solutions of light induced degradation in thin film silicon solar cells. In-situ light-soaking IV measurement techniques are presented. We also present thin film silicon material with silicon nano-quantum dots embedded within amorphous matrix, which shows superior stability during light-soaking. Our results suggest that solar cell using silicon nano-quantum dots in abosrber layer shows superior stability under light soaking, compared to the conventional amorphous silicon solar cell.

Carrier Transport of Quantum Dot LED with Low-Work Function PEIE Polymer

  • Lee, Kyu Seung;Son, Dong Ick;Son, Suyeon;Shin, Dong Heon;Bae, Sukang;Choi, Won Kook
    • Proceedings of the Korean Vacuum Society Conference
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    • 2014.02a
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    • pp.432.2-432.2
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    • 2014
  • Recently, colloidal core/shell type quantum dots lighting-emitting diodes (QDLEDs) have been extensively studied and developed for the future of optoelectronic applications. In the work, we fabricate an inverted CdSe/ZnS quantum dot (QD) based light-emitting diodes (QDLED)[1]. In order to reduce work function of indium tin oxide (ITO) electrode for inverted structure, a very thin (<10 nm) polyethylenimine ethoxylated (PEIE) is used as surface modifier[2] instead of conventional metal oxide electron injection layer. The PEIE layer substantially reduces the work function of ITO electrodes which is estimated to be 3.08 eV by ultraviolet photoemission spectroscopy (UPS). From transmission electron microscopy (TEM) study, CdSe/ZnS QDs are uniformly distributed and formed by a monolayer on PEIE layer. In this inverted QD LED, two kinds of hybrid organic materials, [poly (9,9-di-n-octyl-fluorene-alt-benzothiadiazolo)(F8BT) + poly(N,N'-bis (4-butylphenyl)-N,N'-bis(phenyl)benzidine (poly-TPD)] and [4,4'-N,N'-dicarbazole-biphenyl (CBP) + poly-TPD], were adopted as hole transport layer having high highest occupied molecular orbital (HOMO) level for improving hole transport ability. At a low-operating voltage of 8 V, the device emits orange and red spectral radiation with high brightness up to 2450 and 1420 cd/m2, and luminance efficacy of 1.4 cd/A and 0.89 cd/A, respectively, at 7 V applied bias. Also, the carrier transport mechanisms for the QD LEDs are described by using several models to fit the experimental I-V data.

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Dynamics and Bleaching of Ground State in CdSe/ZnS Quantum Dots

  • Kim, J.H.;Kyhm, K.
    • Journal of the Optical Society of Korea
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    • v.10 no.4
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    • pp.184-187
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    • 2006
  • For resonant excitation of the ground state $1s^e-1S^h_{3/2}$, dynamics of 'the electron-hole pair in a CdSe quantum dot was investigated by degenerate pump-probe measurement. At low e-h pair densities, the decay of $1s^e-1S^h_{3/2}$ state is dominated by radiative recombination. As the number of the electron-hole pairs increases, new decay features become significant. Theoretical comparison suggests this is attributed to the bi-molecular and Auger-type scattering.

Lasing Characteristics of GaAs-Based 1300 nm Wavelength Region InAs Quantum Dot Laser Diode (GaAs 기반 1300 nm 파장대역 InAs 양자점 레이저 다이오드의 발진 특성)

  • Kim, K.W.;Choa, N.K.;Song, J.D.;Lee, J.I.;Park, Jeong-Ho;Lee, Y.J.;Choi, W.J.
    • Journal of the Korean Vacuum Society
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    • v.18 no.4
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    • pp.266-271
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    • 2009
  • We have investigated the lasing characteristics of GaAs-based 1300 nm wavelength region InAs Quantum Dot Laser Diode grown by Migration Enhanced Molecular Beam Epitaxy. Under a pulsed and CW operation, we observed the state switching of lasing wavelength from ground state (1302 nm) to excited state (1206 nm) due to the gain saturation of ground state. Under a pulsed operation, $J_{th}=92A/cm^2$, $\lambda_L=1311\;nm$ and under a CW operation, $J_{th}=247A/cm^2$, $\lambda_L=1320\;nm$.

Effect of Microstructure of Quantum Dot Layer on Electroluminescent Properties of Quantum Dot Light Emitting Devices (양자점 층의 미세구조 형상이 양자점 LED 전계 발광 특성에 미치는 효과)

  • Yoon, Sung-Lyong;Jeon, Minhyon;Lee, Jeon-Kook
    • Korean Journal of Materials Research
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    • v.23 no.8
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    • pp.430-434
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    • 2013
  • Quantum dots(QDs) with their tunable luminescence properties are uniquely suited for use as lumophores in light emitting device. We investigate the microstructural effect on the electroluminescence(EL). Here we report the use of inorganic semiconductors as robust charge transport layers, and demonstrate devices with light emission. We chose mechanically smooth and compositionally amorphous films to prevent electrical shorts. We grew semiconducting oxide films with low free-carrier concentrations to minimize quenching of the QD EL. The hole transport layer(HTL) and electron transport layer(ETL) were chosen to have carrier concentrations and energy-band offsets similar to the QDs so that electron and hole injection into the QD layer was balanced. For the ETL and the HTL, we selected a 40-nm-thick $ZnSnO_x$ with a resistivity of $10{\Omega}{\cdot}cm$, which show bright and uniform emission at a 10 V applied bias. Light emitting uniformity was improved by reducing the rpm of QD spin coating.At a QD concentration of 15.0 mg/mL, we observed bright and uniform electroluminescence at a 12 V applied bias. The significant decrease in QD luminescence can be attributed to the non-uniform QD layers. This suggests that we should control the interface between QD layers and charge transport layers to improve the electroluminescence.

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

  • Dong, Yitong;Parobek, David;Son, Dong Hee
    • Journal of the Korean Ceramic Society
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    • v.55 no.6
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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.