Abstract
We extend the analysis of conductance fluctuations in small disordered metallic systems beyond the conventional thick-lead geometry to thin-lead and isolated geometries. We find that, for the thin-lead geometry, the conductance fluctuations are still given by the ``universal'' value ${e}^{2}$/h, independent of the lead width. In the isolated geometry, the conductance fluctuation is enhanced by a factor (${L}_{\mathrm{in}/\mathrm{L}{)}^{2}\mathrm{\ensuremath{\gg}}1}$ over ${e}^{2}$/h. The typical distance between consecutive peaks and valleys in the structure of conductance fluctuations, both as a function of external magnetic field and of chemical potential, is found to be dramatically reduced in both of these restrictive geometries.
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