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For a pedagogical introduction to quantum information theory, see, e.g., J. Preskill, lecture notes for Caltech Course No. 229, available at http://www.theory.caltech.edu/people/preskill/ph229/. For an overview of experimental achievements, see, e.g., Phys. World 11 (3), 33 (1998). For a survey of more recent developments, see, e.g., J. Mod. Opt. 47, 125 (2000), special issue on quantum information, edited by V. Bužek and D. P. DiVincenzo, and references therein.
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Lecture Notes for Caltech Course No. 229
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Preskill, J.1
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0003186349
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For a pedagogical introduction to quantum information theory, see, e.g., J. Preskill, lecture notes for Caltech Course No. 229, available at http://www.theory.caltech.edu/people/preskill/ph229/. For an overview of experimental achievements, see, e.g., Phys. World 11 (3), 33 (1998). For a survey of more recent developments, see, e.g., J. Mod. Opt. 47, 125 (2000), special issue on quantum information, edited by V. Bužek and D. P. DiVincenzo, and references therein.
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special issue on quantum information, and references therein
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For a pedagogical introduction to quantum information theory, see, e.g., J. Preskill, lecture notes for Caltech Course No. 229, available at http://www.theory.caltech.edu/people/preskill/ph229/. For an overview of experimental achievements, see, e.g., Phys. World 11 (3), 33 (1998). For a survey of more recent developments, see, e.g., J. Mod. Opt. 47, 125 (2000), special issue on quantum information, edited by V. Bužek and D. P. DiVincenzo, and references therein.
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private communication
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H. C. Nägerl (private communication).
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Nägerl, H.C.1
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J. I. Cirac et al. (Ref. [20])
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2 ≪ 1. Although necessary, this condition is not sufficient for the validity of the Jaynes-Cummings Hamiltonian in Eq. (2b), as can be seen from our numerical results in Fig. 4.
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0343992875
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private communication
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D. J. Berkeland (private communication).
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0342686458
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note
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Note that excitation transfer would indeed be possible if one-qubit rotations could also be implemented directly on the motional state. This follows since surrounding a C-NOT gate with Hadamard rotations on both qubits exchanges the role of control and target qubit, and since a sequence of three alternating C-NOT gates is equivalent to the SWAP gate. However, since the motional state cannot be manipulated independently, a SWAP gate cannot be realized with this method alone.
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0343992854
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private communication
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A. Steane (private communication).
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Steane, A.1
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0342686439
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note
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Note that the energy values here are the square roots of the eigenvalues given in Table 2 of [8].
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