Semicircle law (quantum Hall effect)

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The semicircle law, in condensed matter physics, is a mathematical relationship that occurs between quantities measured in the quantum Hall effect. It describes a relationship between the anisotropic and isotropic components of the macroscopic conductivity tensor Template:Mvar, and, when plotted, appears as a semicircle.

The semicircle law was first described theoretically in Dykhne and Ruzin's analysis of the quantum Hall effect as a mixture of 2 phases: a free electron gas, and a free hole gas.[1][2] Mathematically, it states that σxx2+(σxyσxy0)2=(σxx0)2where Template:Mvar is the mean-field Hall conductivity, and Template:Math is a parameter that encodes the classical conductivity of each phase. A similar law also holds for the resistivity.[1]

A convenient reformulation of the law mixes conductivity and resistivity: σxy0=ρxy0(ρxy0)2+(ρxx0)2=e2h(n+12)where Template:Mvar is an integer, the Hall divisor.[3]

Although Dykhne and Ruzin's original analysis assumed little scattering, an assumption that proved empirically unsound, the law holds in the coherent-transport limits commonly observed in experiment.[2][4]

Theoretically, the semicircle law originates from a representation of the modular group Template:Math, which describes a symmetry between different Hall phases. (Note that this is not a symmetry in the conventional sense; there is no conserved current.)[5][6] That group's strong connections to number theory also appear: Hall phase transitions (in a single layer)[5] exhibit a selection rule|pqpq|=1that also governs the Farey sequence.[5][6] Indeed, plots of the semicircle law are also Farey diagrams.

In striped quantum Hall phases, the relationship is slightly more complex, because of the broken symmetry:{σ1σ2+(σhσh0)2=(e2/(2h))2σh0=(N+1/2)e2/hHere Template:Math and Template:Math describe the macroscopic conductivity in directions aligned with and perpendicular to the stripes.[7]

References

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