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note
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Also note that some previous calculations using second order (in the Hubbard U) perturbation theory have not found the subtle effects reported in this paper (see A. Oguri, Phys. Rev. B 63, 115305 (2001), and references therein). The origin of the discrepancy may simply arise from the different accuracy in the many-body techniques employed, but this issue remains to be investigated. However, note that our cancellation of conductance for an odd number of dots leads in a natural manner to the Hubbard insulator limit expected at density one electron per site, as the number of dots grows.
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33646642342
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t″ can be modified by controlling the tunneling to and from the central dot using other appropriate voltages.
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34
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33646638983
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Jerusalem, Israel, edited by D. Gershoni, and references therein
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S. De Franceschi, R. Hanson, W. G. van der Wiel, J. M. Elzerman, J. J. Wijpkema, T. Fujisawa, S. Tarucha, and L. P. Kouwenhoven, cond-mat/0203146
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δ here could represent a bias potential that splits the Kondo peak, similarly as observed by S. De Franceschi, R. Hanson, W. G. van der Wiel, J. M. Elzerman, J. J. Wijpkema, T. Fujisawa, S. Tarucha, and L. P. Kouwenhoven, cond-mat/0203146. Finite-T effects likely reduce the dip depth.
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36
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33646664054
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private communication
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M. F. Crommie (private communication).
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Crommie, M.F.1
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