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1
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0003562493
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Semiconductor spintronics and quantum computation
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edited by D.D. Awschalom, D. Loss, and N. Samarth, (Springer, New York)
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33646641057
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note
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2 via currents through quantum dots in an ESR field (Refs. 24 and 31). However, using an optical detection scheme there is no need for contacting dots with current leads (thus reducing decoherence) and one can benefit from the high sensitivity of photodetectors.
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21
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0001114091
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For dot shapes of lower than circular symmetry, mixing of different band states can become significant. See, e.g., L.-W. Wang, J. Kim, and A. Zunger, Phys. Rev. B 59, 5678 (1999).
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24
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33646652936
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note
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z, we have absorbed the Overhauser field which could possibly arise from dynamically polarized nuclear spins.
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27
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0037092766
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Awschalom, D.D.6
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30
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33646655074
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note
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Excitation of a charged exciton state containing an electron triplet would require an additional energy of ∼40 meV (Ref. 12) and can be excluded by the low laser bandwidth.
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31
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0001679265
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1, similarly as for a single atom [H.J. Kimble, R.J. Cook, and A.L. Wells, Phys. Rev. A 34, 3190 (1986)].
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Kimble, H.J.1
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Flissikowski, T.1
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2342433690
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T. Flissikowski, I.A. Akimov, A. Hundt, and F. Henneberger, Phys. Rev. B 68, 161309(R) (2003); L.M. Woods, T.L. Reinecke, and R. Kotlyar, Phys. Rev. B 69, 125330 (2004).
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Woods, L.M.1
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34
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0035968004
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J.A. Gupta, R. Knobel, N. Samarth, and D.D. Awschalom, Science 292, 2458 (2001); C.E. Pryor and M.E. Flatté, quant-ph/0211160 (unpublished).
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35
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0035968004
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quant-ph/0211160 (unpublished)
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J.A. Gupta, R. Knobel, N. Samarth, and D.D. Awschalom, Science 292, 2458 (2001); C.E. Pryor and M.E. Flatté, quant-ph/0211160 (unpublished).
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Pryor, C.E.1
Flatté, M.E.2
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