By Peter Michler, Alper Kiraz, Christoph Becher, Winston V. Schoenfeld, Pierre M. Petroff (auth.), Prof. Bernhard Kramer (eds.)
This quantity comprises lots of the invited talks of the 2001 assembly of the forged nation Physics component of the Deutsche Physikalische Gesellschaft held from March 26 to 30 in Hamburg, Germany. the subjects lined replicate the current actions during this energetic area of contemporary physics and are hence alleged to flashlight the cutting-edge in condensed topic physics in Germany within the yr 2001.
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Note that the index labelling the dots is not present in the reservoirs – this model contains no conserved quantum number corresponding to spin, unlike previous studies [25,26,27,28]. e. we attach a phase factor eiφ to V2L . The level broadening is deﬁned by Γjr = 2π|Vjr |2 ρ0 , where ρ0 is the density of states in the leads, which we assume to be constant in the energy range of interest. The total broadening of each level is therefore given by Γ = ΓjL + ΓjR . Since both levels overlap with the reservoirs, they have an eﬀective overlap matrix element ∆, which induces a level splitting δ˜ = δ 2 + |∆|2 where c1 ...
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