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By Andreas Glatz, Veniamin I. Kozub, Valerii M. Vinokur

The booklet displays medical advancements within the physics of metal compound dependent nanodevices awarded on the NATO-sponsored Workshop on nanophysics held in Russia in the summertime of 2003. this system tackles the main attractive difficulties. It brings jointly experts and offers a chance for younger researchers from the companion nations to have interaction with them and get actively interested by the main beautiful and promising interdisciplinary region of latest condensed topic physics.

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B 67, 174402 (2003). 9. B. D. Kent, D. Z. J. H. Koch, Phys. Rev. Lett. 91, 067203 (2003). 10. S. Urazhdin, H. P. , and J. Bass, Appl. Phys. Lett. 83, 114 (2003). 11. S. O. P. , and J. Bass, Phys. Rev. Lett. 91, 146803 (2003). 12. S. Urazhdin, cond-mat/0308320. 13. If we follow the reversible switching peak to very large I and H, the dwell times τP and τP extrapolate to values smaller than any plausible microscopic attempt time. At that point the magnetization dynamics no longer produce telegraph noise, but become more complicated.

S. , Phys. Rev. B 63, 115109 (2001). 5. V. Ambegaokar, U. Eckern, and G. Sch¨ on, Phys. Rev. Lett. 48, 1745 (1982). 6. I. S. Beloborodov and A. V. Andreev, in preparation. 7. B. L. Altshuler and A. G. Aronov, in Electron-Electron Interaction in Disordered Systems, ed. by A. L. Efros and M. Pollak, North-Holland, Amsterdam (1985). 8. I. S. Beloborodov and K. B. Efetov, Phys. Rev. Lett. 82, 3332, (1999). 9. A. A. Abrikosov, L. P. Gorkov, I. E. Dzyaloshinski, Methods of quantum field theory in statistical physics, Dover Publications, New York 10.

The term H interaction inside and between the grains. It has the following form 2 ˆc = e H 2 −1 n ˆ i Cij n ˆj , (6) ij where Cij is the capacitance matrix and n ˆ i is the operator of electron number in the i-th grain. In the regime under consideration one can neglect the coordinate dependence of a single grain diffusion propagator. The electron hopping between the grains can be included using the diagrammatic technique developed in Refs. [8, 4], which we outline below. The electron motion in a random impurity potential within a single grain can be considered using the standard diagrammatic techniques described, for example in Ref.

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