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Quantum Control in Semiconductor Quantum Dots Yan-Ten Lu Physics, NCKU Basic Requirements 1. Representation of qubits 2. Controllable unitary evolution 3. Preparation of initial qubit states 4. Measurement of final qubit states Representation of qubits Single photon Cavity QED Trapped ions Nuclear spins Solid state devices C11H5F5O2Fe 15 = 3 x 5 -- Realization of Shor Algorithm (1994) by I. Chuang (2001), IBM Almaden Time Constants (Nielsen & Chuang p.278) system nuclear spin electron spin ion trap (In+) electron (Au) electron (GaAs) Quantum dot Optical cavity Microwave cavity Coh. T 10+2 10-3 10-1 10-8 10-10 10-6 10-5 1 Op. T 10-3 10-7 10-14 10-14 10-13 10-9 10-14 10-4 No Op 10+5 10+4 10+13 10+6 10+3 10+3 10+9 10+4 Quantum Dots Charge (current) Spin Exciton 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 105 – 106 atoms. InAs/GaAs, S.P. Gua, et. al. APL 1997 C. Pryor, PRL 1998 Charged quantum dots, Nielson & Chuang, p.344 Spin of a quantum dot Loss & DiVinceenzo, PRA, 1998 H s (t ) J (t )S1 S2 Exciton in Semiconductor E e V (re , rh ) 2 r 0.05 mo k Eb = 6 meV Exciton in Q-dot Eb e (re ) V (re , rh ) h (rh ) Eb = 20 meV 2 Energy levels of multiple excitons, A. Barenco, PRB, 1995 L.Sham, PRL 2001, PRB 2002 Ee - Eh = 1.6926 Eex = 1.6724 Tcoh = 30 ps H. Ando, PRL 2001 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 E Combined laser pulses Excited by a left polarized beam Two-pulse combination E (t ) Eo e (t / ) o 1 2 e i 0 t E1e ( t / 1 ) 2 i1t i e Fidelity Test 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) M. Bayer, Science 2001 K.R. Brown, et. al. PRA 2001