Real wires with islands



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Next: Discussion and Conclusion Up: Conductance and conductance fluctuations Previous: The Influence of

Real wires with islands

  So far we have examined separately the effects of boundary roughness and islands on the quantum wire conductance. Real wires with islands have both types of disorder. The geometry of the system used for the calculation of the conductance is the same as in the case of real wires without islands, shown at the top of Fig. 2.

  
Figure 10: The average conductance and the conductance fluctuations as function of energy for real wire with islands, p=5(black full line), for wire lengths and . These results can be compared with the results for the case of real wire without islands (i.e. wire with rough edges), , , and perfect wire with islands of concentration and , . For wire length , and are virtually the same, so only is shown, whereas for both averages are shown. Number of samples are: and .

Some results for the average conductance and fluctuations as functions of energy are shown in Fig. 10 for two lengths of wire, and . The average conductance for both regimes shows no features, just a monotonically rising curve which bends and falls off near the band centre. The presence of both types of disorder causes a further decrease of the conductance when compared with a wire with only one type of disorder. One can say that the influence of islands is dominant for energies near the band edge, whereas the influence of edge roughness becomes dominant towards the band centre. Any feature of the conductance quantization for a single sample is quickly destroyed by the presence of both types of disorder. The conductance fluctuations for nearly ballistic samples () have similar values to the fluctuations for the case of a real wire without islands, except for energies near the band edge. However, as the wire length increases the conductance fluctuations for a real wire with islands decreases faster then for the case without islands. This is because strong localization sets in sooner in the presence of islands. It was found in Nikolic and MacKinnon (1993) that the localization length of real wires with islands is usually about half of the localization length of real wires without islands (case of island concentration).

The conductance fluctuations as a function of length behave like the conductance fluctuations for the case of a perfect wire with islands for energies near the band edge, but for higher energies they are similar to the case of real wires without islands.



next up previous
Next: Discussion and Conclusion Up: Conductance and conductance fluctuations Previous: The Influence of



Angus MacKinnon
Fri Nov 18 13:59:27 gmt 1994