Résumé
Mesoscopic circuits cooled down to low temperatures witness marked non-local effects in their transport properties because of electron coherenceĝ€"electron wavefunctions spread over the sample and correlate its different parts. One of the consequences is that, in one dimension, the maximum d.c. conductance is quantized in steps of e 2 /h. Here we extend the concept of e 2 /huniversal quantized resistance'to the a.c. regime. We analyse the coherent quantum resistanc-capacitance circuit comprising a cavity capacitively coupled to a gate and connected by means of a single spin-polarized channel to a reservoir lead. We show that, as a result of the Coulomb interaction and global phase coherence, the charge relaxation resistance Rq is identical for weak and large transmissions and that it smoothly changes from h/2e 2 to h/e 2 when the frequency exceeds the level spacing of the cavity. For large cavities, we relate the resistance h/e 2 to the Korring-Shiba relation of the Kondo model. Finally, we introduce a larger class of models with a universal charge relaxation resistance.
| langue originale | Anglais |
|---|---|
| Pages (de - à) | 697-701 |
| Nombre de pages | 5 |
| journal | Nature Physics |
| Volume | 6 |
| Numéro de publication | 9 |
| Les DOIs | |
| état | Publié - 1 janv. 2010 |
| Modification externe | Oui |
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