Advances in Solid State Physics by Rolf Haug PDF

By Rolf Haug

ISBN-10: 3540382348

ISBN-13: 9783540382348

The current quantity forty six of Advances in Solid-State Physics comprises 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 quite a few symposia are incorporated. each one of these have been geared up collaboratively through a number of of the divisions of the Arbeitskreis. The booklet provides, to some degree, the prestige of the sector of solid-state physics in 2006 not just in Germany but additionally across the world.

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Minimization of the total elastic strain is the driving force for the selforganized formation of QDs using the widely applied Stranski-Krastanow (SK) growth mode [8]. The equilibrium shape of free-standing coherently strained QDs in zincblende materials was modeled to adopt either the form of a peaked or a truncated pyramid with flat top and bottom interfaces on (001)oriented substrates [9, 10], in agreement with experimental findings [11–13]. For capped QDs a large variety of shapes and compositions is reported, due to the strong impact of the non-equilibrium overgrowth procedure.

Emary, M. Kindermann, Phys. Rev. Lett. 93, 020501 (2004). [13] V. N. Golovach, A. V. Khaetskii, D. Loss, Phys. Rev. Lett. 93, 016601 (2004). [14] J. M. Elzerman, R. Hanson, L. H. Willems van Beveren, B. Witkamp, L. M. K. Vandersypen, L. P. Kouwenhoven, Nature 430, 431 (2004). [15] M. Kroutvar, Y. Ducommun, D. Heiss, M. Bichler, D. Schuh, G. Abstreiter, J. J. Finley, Nature 432, 81 (2004). [16] J. Schliemann, A. Khaetskii, D. Loss, J. : Condens. Matter 15, 1809 (2003). [17] G. Burkard, D. Loss, D.

With this for a time tm . Finally we adiabatically switch back to J the |+ state goes to the singlet S(1, 1), and the |− state goes to the S z = 0 triplet T0 (1, 1). Read-out of the singlet and triplet may then be achieved via switching to large positive detuning: the S(1, 1) state goes over to the S(0, 2) Quantum-Dot Spin Qubit and Hyperfine Interaction 25 Fig. 2. In this figure the pulse-sequence for one measurement in the basis |± is explained. (a) The level diagram for the two-electron spin states (sweeping = ES(1,1) − ES(0,2) with ES(1,1) + ES(0,2) held constant).

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Advances in Solid State Physics by Rolf Haug

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