• Resonant Tunning Through Quantum Dot Array

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    • 1.8.2    Electrochemical Assembly
      Highly ordered arrays of quantum dots may also be self-assembled by electrochemical techniques. A template is created by causing and ionic reaction at an electrolyte-metal interface which results in the spontaneous assembly of nanostructures, including quantum dots, onto the metal which is then used as a mask for mesa-etching these nanostructures on a chosen substrate.
      1.8.3    Bulk-manufacture
      Conventional, small-scale quantum dot manufacturing relies on a process called “high temperature dual injection” which is impractical for most commercial applications that require large quantities of quantum dots.
      A reproducible method for creating larger quantities of consistent, high-quality quantum dots involves producing nano-particles from chemical precursors in the presence of a molecular clusters compound under conditions whereby the integrity of the molecular clusters is maintained and acts as a prefabricated seed template. Individual molecules of a clusters compound act as a seed or nucleation point upon which nano- particle growth can be initiated. In this way, a high temperature nucleation step is not necessary to initiate nano-particle growth because suitable nucleation sites are already provided in the system by the molecular clusters. A significant advantage of this method is that it is highly scalable.
      Recently a consortium of U.S. and Dutch companies reported a “milestone” in high volume quantum dot manufacturing by applying the traditional high temperature dual injection method to a flow system. However as of 2011, applications using bulk- manufactured quantum dots are scarcely available.
      1.8.4    Cadmium-free quantum dots
      Cadmium-free quantum dots are also called “CFQD”. In many regions of the world there is now a a restriction or ban on the use of heavy metals in many household goods which means that most cadmium based quantum. Dots are unusable for consumer- goods applications.
      For commercial viability, a range of restricted, heavy metal-free quantum dots has been developed showing bright emissions in the visible and near infra-red region of the spectrum and have similar optical properties to those of CdSe quantum dots.
      Cadmium and other restricted heavy metals used in conventional quantum dots are of a major concern in commercial applications. For Quantum Dots to be commercially viable in many applications they must not contain cadmium or other restricted metal elements.
      A new type of CFQD can be made from rare earth (RE) doped oxide colloidal phosphor nano-particles. Unlike semiconductor nano-particles, excitation was due to UV absorption of hopst material, which is same for different RE doped materials using same host. Multiplexing applications can be thus realized. The emission depends on the type of RE, which enables very large stokes shift and is narrower than CdSe QDs. The synthesis is aqueous based, which eliminated issues of water solubility for biological applications. The oxide surface might be easier for chemical fictionalization more and chemically stable in various environments. Some reports exist concerning the use of such phosphor nano-particles on biological targeting and imaging.
      1.9    Optical properties of quantum dots
      An immediate optical feature of colloidal qantum dots is their coloration. While the material which makes up a quantum dot defines its intrinsic energy signature, the nanocrystal”s quantum confined size is more significant at energies near the band gap. Thus quantum dots of the same material, but with different sizes, camemit light of different colors. The physical reason is the quantum confinement effect.
      The lager the dot, the redder (lower energy) its fluorescence spectrum.
      Conversely, smaller dots emit bluer (higher energy) light. The coloration is directly related to the energy levels of the quantum dot. Quantitatively speaking, the band gap energy that determines the energy (and hence color) of the fluoresencnt light is inversely proportional to the size of quantum dot. Lager quantum dots have more energy level which also more closely spaced. This allows the quantum dot to absorb photons containing less energy, i.e those closer to the red end of the spectrum. Recent articles in nanotechnology and in other journals have begun to suggest that the shape of the quantum dot may be a factor in the coloration as well, but as yet not enough information is available. Furthermore, it was shown that the lifetime of fluorescence is determined by the size of the quantum dot. Lager dots have more closely spaced energy level in which the electron-hole pair can be trapped. Therefore, electron-hole pairs in larger dots live longer causing larger dots to show a longer lifetime
      As with any crystalline semiconductors , a quantum dots electronic wave function extend over the crystal lattice similar to a molecule, a quantum dot has both a quantize energy spectrum and a quantized density of electronics state near the edge of the band gap.
      Quantum dots can be synthesize with larger (thicker) shells (CdSe qdots with CdS shells.) the shell thickness has shown direct correlation to the lifetime and emission intensity.
      1.10    Application of quantum dots
      Quantum dots are particularly significant for optical applications due to their high extension co-efficient. In electronics application they have been proven to operate like a single-electron transistors and show the Coulomb blockade effect.
      Quantum dot have also been suggested as implementations of qubits for quantum information processing.
      The ability to tune the size of quantum dots have advantageous for many applications. For instance, larger quantum dots have a greater spectrum-shift towards red compared to smaller dots , and exhibit less pronounced quantum properties. Conversely, the smaller particle allows one to take advantage of more subtle quantum effects.
      Researchers at Los Alamos National Laboratory have developed a wireless device that efficiently produces visible light, through energy transfer from thin layers of quantum wells to crystals above the layers.
      Being zero dimensional, quantum dots have a shaper density of state than higher- dimensional structures. As a result, they have superior transport and optical properties, and are being researched for use in diode lasers, amplifiers, and biological sensors. Quantum dots may be excited within a locally enhanced electromagnetic field produced by gold nano- particles, which can then be observed from the surface Plasmon resonance in the photo luminescent excitation spectrum of (CdSe) ZnS nanocrystal. High –quality quantum dots are well suited for optical encoding and multiplexing applications due to their broad excitation profiles and narrow/symmetrical emission spectra. The new generations of quantum dots have far-reaching potential for the study of intracellular processes at the single-molecule level, high-resolution cellular imaging, long-term in vivo observation of cell trafficking, tumor targeting, and diagnostics. Measurement of the spin and other properties therein can be made. With several entangle quantum dots or qubits plus a way of performing operations; quantum calculations and the computers that would perform them might be possible.
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    • ABSRACT - [ Total Page(s): 1 ]Abstract coming soon ... Continue reading---

         

      CHAPTER TWO - [ Total Page(s): 2 ]CHAPTER TWORESONANT TUNNELING THROUGH QUANTUM DOT ARRAY PROCESSE is incident on a potential barrier of height V0 . Classically the electron is reflected when E< V0, but quantum mechanically there is a certain probability that the electron is transmitted through the barrier.Tunneling is a purely quantum mechanical phenomena which enables electrons to penetrate potential barriers even though it is classically forbidden. The scheme is illustrated in Figure above. Classically the electron would be r ... Continue reading---

         

      CHAPTER THREE - [ Total Page(s): 9 ]The Hamiltonian equation above is a representation of Quantum dot array i.e 1- Darray of N coupled dots index from left to right as 1- N. looking at the energy of a quantum dot confined dots (20 energy states been treated as a single quantum systemFrom the equationεka is the energy levels in leadsεia is the ith dot of the energy Ui is theith inter- dot repulsion and the inter-dot coupling between theith dot and its rightneighbor (the (i+1)th dot)V L and V R are the tunnels matrix element c ... Continue reading---

         

      CHAPTER FOUR - [ Total Page(s): 2 ]CHAPTER FOURDISCUSSION OF RESULTSFrom the matrices gotten in the previous chapter, it is seen that the diagonal four-by-four matrices are proportional to the partition function Z.In Eq. (2), En, is the energy of many-body state (n, i), the ith of the n-particle states, RL ,®ij are the transition rates between state (n,i) and (n-I,j) by losing or getting one electron through the left (right) lead, and peqn,I is the occupation probability of state (n,i) at equilibriumEquation (2) is basically t ... Continue reading---

         

      CHAPTER FIVE - [ Total Page(s): 3 ]CHAPTER FIVECONCLUSION ... Continue reading---

         

      REFRENCES - [ Total Page(s): 1 ]REFERENCESFriedlander, Michael W. 2000 A Thin Cosmic Rain: Particles from Outer Space (Cambridge:Harvard University Press).Watson, Alan 2001 “Ultra High Energy Cosmic Rays: What we Know Now and What the FutureHolds,” in Relativistic Astrophysics: 20th Texas Symposium (AIP Conference Procedings, volume 586, J. C. Wheeler and H. Martel (eds.) American Institure of Physics, pp. 817–826. (The original abstract was different from the published abstract)Anderson, Carl D ... Continue reading---