We show from exact calculations that a simple tight-binding Hamiltonian with diagonal disorder and long-range hopping integrals, falling off as a power µ of the inter-site separation, correctly describes the experimentally observed amplitude (close to the value of an ordered ring) and flux-periodicity (hc/e) of persistent currents in single-isolated-diffusive normal metal rings of mesoscopic size. Long-range hopping integrals tend to delocalize the electrons even in the presence of disorder resulting orders of magnitude enhancement of persistent current relative to earlier predictions.
Keywords: Model Calculations, MagnetotransportThe phenomenon of persistent current in mesoscopic normal metal rings has generated a lot of excitement as well as controversy over the past years. In a pioneering work, Büttiker, Imry and Landauer [1] predicted that, even in the presence of disorder, an isolated 1D metallic ring threaded by magnetic flux φ can support an equilibrium persistent current with periodicity φ 0 = ch/e, the flux quantum. Later, experimental observations confirm the existence of persistent currents in isolated mesoscopic rings. However, these experiments yield many results that are not well-understood theoretically even today [2,3,4,5,6,7,8,9,10,11,12,13]. The results of the single loop experiments are significantly different from those for the ensemble of isolated loops. Persistent currents with expected φ 0 periodicity have been observed in isolated single Au rings [14] and in a GaAs-AlGaAs ring [15]. Levy et al. [16] found oscillations with period φ 0 /2 rather than φ 0 in an ensemble of 10 7 independent Cu rings. Similar φ 0 /2 oscillations were also reported for an ensemble of disconnected 10 5 Ag rings [17] as well as for an array of 10 5 isolated GaAs-AlGaAs rings [18]. In a recent experiment, Jariwala et al.[19] obtained both φ 0 and φ 0 /2 periodic persistent currents in an array of thirty diffusive mesoscopic Au rings. Except for the case of the nearly ballistic GaAs-AlGaAs ring [15], all the measured currents are in general one or two orders of magnitude larger than those expected from the theory [2,3,4,5,6,7,8,9,10,11,12]. The diamagnetic response of the measured φ 0 /2 oscillations of ensembleaveraged persistent currents near zero magnetic field also contrasts with most predictions [8,9].Free electron theory predicts that at T = 0, an or- * Corresponding author: Santanu K. Maiti E-mail: santanu@cmp.saha.ernet.in dered 1D metallic ring threaded by magnetic flux φ supports persistent current with maximum amplitude I 0 = ev F /L, where v F is the Fermi velocity and L is the circumference of the ring. Metals are intrinsically disordered which tends to decrease the persistent current, and the calculations show that the disorder-averaged current < I > crucially depends on the choice of the ensemble [3,4,5]. The magnitude of the current < I 2 > 1/2 is however insensitive to the averaging issues, and is of the order of I 0 l/L, l being the elastic mean free path of the electrons. This expression...