Abstract
The effect of a strong magnetic field on the persistent current and current-current correlations in the Laughlin geometry are discussed. Due to the violation of time-reversal symmetry a single disordered sample may carry a current even in the absence of a threading flux. Once one averages over many realizations this current disappears. A theory is presented for the current-current correlations in the presence of a strong magnetic field and compared to the results of a numerical calculation. The results fit for the bulk states while discrepancies appear for edge states.
| Original language | English |
|---|---|
| Pages (from-to) | 14448-14455 |
| Number of pages | 8 |
| Journal | Physical Review B-Condensed Matter |
| Volume | 49 |
| Issue number | 20 |
| DOIs | |
| State | Published - 1994 |
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