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Summary

In conclusion, a coherent system of one or more weakly coupled quantum dots with Coulomb interaction can be well described using Green's functions of a probabilistic nature. In a double dot, the modes of the individual dots are coupled together. The resulting level repulsion can lead to a complex form of the Ohmic conductance and the current. Regions of negative differential conductance are likely to occur. The Ohmic conductance through two dots with multiple levels is dominated by the matching energy levels.

The maximum conductance through a double dot tex2html_wrap_inline1192 is reached at low temperatures in the symmetric case of aligned levels tex2html_wrap_inline1342, identical coupling to the reservoirs tex2html_wrap_inline1328 and tex2html_wrap_inline1358.

The peaks that occur in the current as the gate potential of one of the dots is varied while keeping the voltage bias across the dots fixed have a Lorentzian line shape with a width at least as large as the combined broadening of the individual dot levels.


references521

  figure638
Figure 1: Current and associated differential conductance through a dot with a spin-split level for the various approximation schemes (tex2html_wrap_inline1196, tex2html_wrap_inline1376, tex2html_wrap_inline1378, tex2html_wrap_inline1380, tex2html_wrap_inline1382)

  figure645
Figure 2: Ohmic conductance through a dot with a spin-split level for the various approximation schemes (tex2html_wrap_inline1376, tex2html_wrap_inline1378, tex2html_wrap_inline1380).

  figure652
Figure 3: Occupation of a dot with a spin-split level for the various approximation schemes (tex2html_wrap_inline1376, tex2html_wrap_inline1378, tex2html_wrap_inline1380). The two sets of curves refer to the occupation of the tex2html_wrap_inline1152 and tex2html_wrap_inline1154 states.

  figure659
Figure 4: Ohmic conductance through two dots each with a level for both spins, using various coupling constants tex2html_wrap_inline1214 (tex2html_wrap_inline1402, tex2html_wrap_inline1376, tex2html_wrap_inline1406, tex2html_wrap_inline1408, tex2html_wrap_inline1410, tex2html_wrap_inline1412). In the occupation plots the solid lines correspond to the states of spin tex2html_wrap_inline1152, the dotted lines to the states of spin tex2html_wrap_inline1154.

  figure668
Figure 5: Current through two dots each with a level for both spins, using various coupling constants tex2html_wrap_inline1214 (tex2html_wrap_inline1420, tex2html_wrap_inline1402, tex2html_wrap_inline1376, tex2html_wrap_inline1406, tex2html_wrap_inline1408, tex2html_wrap_inline1410, tex2html_wrap_inline1412). In the occupation plots the solid lines correspond to the states of spin tex2html_wrap_inline1152, the dotted lines to the states of spin tex2html_wrap_inline1154.

  figure677
Figure 6: Ohmic conductance through two dots with multiple levels in the limit of small coupling tex2html_wrap_inline1438 (tex2html_wrap_inline1440, tex2html_wrap_inline1442, tex2html_wrap_inline1444, tex2html_wrap_inline1446, tex2html_wrap_inline1328). The empty and filled circles indicate the positions at which the average occupation increases by one for dot 1 and 2 respectively.


next up previous
Up: Coherent tunnelling through two Previous: Multi-Level Dots

Angus MacKinnon - Aonghus Mac Fhionghuin Fri Nov 8 17:44:15 gmt 1996