By Prof. Dr. Rolf Haug (auth.)

ISBN-10: 3540382348

ISBN-13: 9783540382348

ISBN-10: 3540382356

ISBN-13: 9783540382355

The current quantity forty six of Advances in sturdy kingdom Physics includes the written types of chosen invited lectures from the spring assembly of the Arbeitskreis Festkörperphysik of the Deutsche Physikalische Gesellschaft which was once held from 27 to 31 March 2006 in Dresden, Germany. Many topical talks given on the a number of symposia are incorporated. each one of these have been geared up collaboratively by means of a number of of the divisions of the Arbeitskreis. The topis variety from zero-dimensional physics in quantum dots, molecules and nanoparticles over one-dimensional physics in nanowires and 1d platforms to extra utilized matters like optoelectronics and fabrics technology in skinny movies. The contributions span the entire width of solid-state physics from actually simple technology to applications.

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M ment, it is the measurement outcome |− that leads to narrowing. Thus, before each measurement ωi is chosen to maximize the probability Pω−i to measure |− . The reason that ωi must be adapted and that one should not keep measuring at the same driving frequency is that the measurement outcome |+ causes a dip in ρI (x) at the position where Lωi (x) has its peak and since Pω−i is the overlap of ρI (x) and Lωi (x), this causes Pω−i to diminish with each measurement. To see what is a typical measurement history for such an adaptive scheme we have performed simulations.

A. Laird, A. Yacoby, M. D. Lukin, C. M. Marcus, M. P. Hanson, A. C. Gossard, Science 309, 2180–2184 (2005) [19] R. Schleser, E. Ruh, T. Ihn, K. Ensslin, D. C. Driscoll, A. C. Gossard, Appl. Phys. Lett. 85, 2005–2007 (2004) [20] L. M. K. Vandersypen, J. M. Elzerman, R. N. Schouten, L. H. Willems van Beveren, R. Hanson, L. P. Kouwenhoven, Appl. Phys. Lett. 85, 4394–4396 (2004) [21] D. A. Bagrets, Y. V. Nazarov, Phys. Rev. B 67, 085316 (2003) [22] S. Gustavsson, R. Leturcq, B. Simovič, R. Schleser, T.

6b can be understood as follows. For eV /2 ≈ i , the eﬀective tunneling rates are functions of the value of the Fermi distribution at i . , 42 S. Gustavsson et al. ΓL fL ( i ) in (2)) changes from 0 to ΓL . Considering the tunneling rate of ΓL , the the right lead constant in this region, and with the condition ΓR asymmetry of the coupling will then change continuously from −1 to 0 and 1, giving this strong reduction of the normalized central moments to 1/2 and 1/4 when the asymmetry is close to zero.

### Advances in Solid State Physics by Prof. Dr. Rolf Haug (auth.)

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