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85034123821
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note
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This linear lever arm picture is exact only as long as the dots are uncharged. However, simulations with a 1D-Poisson solver show that for the relevant charge densities, it is appropriate to use this argument for the calculation of the energy levels of the dots.
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11
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85034137166
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note
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1 both the p states and the wetting layer are (at sufficiently high frequencies) affected in the same way as here the s states.
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13
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0001207033
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The effective distance between the dots and the back contact is slightly different from the geometric value due to a spreading of charge from the back contact. In addition, the strain field from the dot modifies the conduction band. See J. H. Davies, J. Appl. Phys. 84, 1358 (1998).
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Davies, J.H.1
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85034131891
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note
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First indications for this effect can be observed as a difference between the charging and the decharging signal.
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16
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J. Bardeen, Phys. Rev. Lett. 6, 57 (1961); E. O. Kane, in Tunneling Phenomena in Solids, edited by E. Burstein and S. Lundqvist (Plenum, New York, 1969).
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edited by E. Burstein and S. Lundqvist Plenum, New York
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Kane, E.O.1
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I. Lundström and C. Svensson, J. Appl. Phys. 43, 5045 (1972); A. O. Govorov and W. Hansen, Phys. Rev. B 58, 12980 (1998).
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