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Quantum Control in Semiconductor Quantum Dots Yan-Ten Lu Physics, NCKU
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Basic Requirements 1. Representation of qubits 2. Controllable unitary evolution 3. Preparation of initial qubit states 4. Measurement of final qubit states
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Representation of qubits Single photon Cavity QED Trapped ions Nuclear spins Solid state devices
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15 = 3 x 5 -- Realization of Shor Algorithm (1994) by I. Chuang (2001), IBM Almaden C 11 H 5 F 5 O 2 Fe
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Time Constants (Nielsen & Chuang p.278) systemCoh. TOp. TNo Op nuclear spin10+210-310+5 electron spin10-310-710+4 ion trap (In+)10-110-1410+13 electron (Au)10-810-1410+6 electron (GaAs)10-1010-1310+3 Quantum dot10-610-910+3 Optical cavity10-510-1410+9 Microwave cavity110-410+4
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Quantum Dots Charge (current) Spin Exciton
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What is a quantum dot? In a semiconductor quantum dot, the electronic levels have a density of states characteristic of a single atom. Yet, the dots is a mesoscopic system, the quantization of electronic levels is realized within a system of 10 5 – 10 6 atoms.
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InAs/GaAs, S.P. Gua, et. al. APL 1997
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C. Pryor, PRL 1998
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Charged quantum dots, Nielson & Chuang, p.344
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Spin of a quantum dot Loss & DiVinceenzo, PRA, 1998
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Exciton in Semiconductor k E E b = 6 meV
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Exciton in Q-dot E b = 20 meV
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Energy levels of multiple excitons, A. Barenco, PRB, 1995
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L.Sham, PRL 2001, PRB 2002
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E e - E h = 1.6926 E ex = 1.6724 T coh = 30 ps H. Ando, PRL 2001
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Time Scale Consideration Pusle duration of operation laser beam must be less than coherence time Pulse duration of laser beam must be long enough to ensure Combined laser pulses
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Excited by a left polarized beam
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Two-pulse combination
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Fidelity Test
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What We can do ? More detail study of fidelity dependence on the shape of laser pulse. Applied to system of coupled quantum dots (1-d and 2-d)
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M. Bayer, Science 2001
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K.R. Brown, et. al. PRA 2001
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