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Overview of First Presentation Laser Types of Laser Quantum DL Basic Components of QDL Types of QDL Theory of QDL Application
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Non-traditional semiconductor Crystals composed of periodic groups of II-VI, III-V, or IV-VI materials Range from 2-10 nanometres (10-50 atoms) in diameter An electromagnetic radiation emitter with an easily tunable band gap 0 degrees of freedom
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Number of free dimensions StructureQuantum Confinement 3BulkNone 2Quantum Well 1 1Quantum Wire 2 0Quantum Dot 3 Structures and energy levels in quantum confined systems
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There are three main ways to confine excitons in semiconductors: ◦ Lithography ◦ Colloidal synthesis ◦ Epitaxy: Patterned Growth Self-Organized Growth 4 2. Fabrication of Quantum Dots
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Light Amplification by Stimulated Emission of Radiation. Laser light is monochromatic, coherent, and moves in the same direction.
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Lasers are commonly designated by the type of lasing material employed: Gas lasers: The most important are CO2 and excimer lasers (derived from “excited dimer”: ArF, KrF, XeCl). Moreover, there are also the heliumneon and argon-ion lasers. Liquid lasers: The medium is a dye solution, as a result of which the colour of the laser light can be varied over a wide range.
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Solid-state type lasers: The most important one is the neodymium-YAG laser. The medium in this case is a synthetically produced monocrystal, yttrium-aluminium- garnet, in which some yttrium ions have been replaced by neodymium ions. Semi-conductor/diode lasers: After quantum dot laser, The latest laser types which generate light effectively from the smallest space
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A quantum dot laser is a semiconductor laser that uses quantum dots as the active laser medium in its light emitting region. ◦ Due to the tight confinement of charge carriers in quantum dots, they exhibit an electronic structure similar to atoms.
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DEVELOPMENT OF QDL
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An ideal QDL consists of a 3D-array of dots with equal size and shape Surrounded by a higher band-gap material ◦ confines the injected carriers. Embedded in an optical waveguide ◦ Consists lower and upper cladding layers (n-doped and p-doped shields)
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Wavelength of light determined by the energy levels not by bandgap energy: improved performance & increased flexibility to adjust the wavelength Maximum material gain
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Low threshold High output power Large modulation bandwidth Superior temperature stability
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High speed quantum dot lasers Directly modulated quantum dot lasers Mode-Locked Quantum Dot Lasers InP Based Quantum Dot Lasers
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High power Quantum Dot lasers QD lasers for Coolerless Pump Sources Single Mode Tapered Lasers
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High speed quantum dot lasers Advantages Directly Modulated Quantum Dot Lasers Datacom application Rate of 10Gb/s Mode-Locked Quantum Dot Lasers Short optical pulses Narrow spectral width Broad gain spectrum InP Based Quantum Dot Lasers Low emission wavelength Wide temperature range Used for data transmission
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High power Quantum Dot lasers Advantages QD lasers for Coolerless Pump Sources Size reduced quantum dot Single Mode Tapered Lasers Small wave length shift Temperature insensitivity
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The potential energy region defined by
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Inside the well Schrödinger equation is identical that of free particle and reduces to =0=0
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more precisely to three independent equation of the form The most general solution of x equation is given by
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The boundary condition so that X(x) is given by for
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The additional boundary condition is applied x=L gives Implying that, which finally gives
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The solution has the same form each independent coordinate giving for with Or
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QD Lasers Microwave/Millimeter wave transmission with optical fibers Datacom network Telecom network Optics
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25 Photovoltaic devices: solar cells Biology : biosensors, imaging Light emitting diodes: LEDs Quantum computation Flat-panel displays Memory elements Photodetectors 25 Applications
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Gerald B. Stringfellow (1999). Organometallic Vapor-Phase Epitaxy: Theory and Practice (2nd ed.). Academic Press Betul Arda, Huizi Diwu. Department of Electrical and Computer Engineering University of Rochester http://www.raunvis.hi.is/~ario/ntlj/Quantum_Dot_Lasers_BA.pdf http://www.nanoscienceworks.org H. Goronkin, P. Allmen, R. Tsui, T. Zhu, “Functional Nanoscale Devices”, ch.5. N. N. Ledentsov, “Quantum Dot Heterostructures: Fabrication, Properties, Lasers” D. Bimberg, G. Fiol, M. kuntz et al. “High speed nanophotonic devices based on quantum dots.”phys D. Bimberg, M. Grundmann, N. Ledenstov, “Quantum Dot Heterostructures” Particle in a box figures, http://xbeams.chem.yale.edu/~batista/vvv/node4.html Retrieved in 19.05.2010
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