Giant persistent current in free-electron model with flat Fermi surface

Details Giant persistent current in free-electron model with flat Fermi surface Giant persistent current in free-electron model with flat Fermi surface

1996-12-31

arxiv.org/abs/cond-mat/9612253v3

Physics

Condensed Matter

18 revtex preprint pages + 4 ps figures

Scientific paper

For the first time the persistent current in a 2D free-electron system has been calculated analytically. The tight binding model is considered on a square lattice with filling factor 1/2. The array has a shape of rectangle with boundary conditions in both directions twisted by $2\pi\phi_x$ and $2\pi\phi_y$. The components of the twist are associated with two components of the magnetic flux in torus geometry. An analytical expression is obtained for the energy and for the components of the persistent current (PC) at a given flux and temperature. It is shown that at zero temperature the PC density is proportional to the vector potential with the coefficient which does not depend on the size of the system. This happens because the Fermi surface for a square lattice at filling factor 1/2 is flat. Both the energy and the PC are periodic functions of the two flux components with the periods $\phi_0/q$ and $\phi_0/s$ where $\phi_0=hc/e$, and $q$ and $s$ are integers which depend on the aspect ratio of the rectangle. The magnitude of PC is the same as in superconductors. Therefore, a 3D system constructed from a macroscopic number of isolated coaxial cylinders at zero temperature reminds the London's superconductor. It exhibits the quantization of trapped flux as well as the Meissner effect. However, all the phenomena are of a mesoscopic nature. The critical field $H_c$ decays with an effective size of the system, $H_c\sim 1/R_{ef}$. The magnitude of PC decays with $T$ as $\exp(-\pi TR_{ef}/2at)$, where $t$ is the hopping amplitude and $a$ is the lattice constant.

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