What Happens to the Integer Quantum Hall Effect in Three Dimensions?
Chapter in Supersymmetry and Trace Formulae, Springer Nature 370 (1999) 75-83
Quantum Hall plateau transitions in disordered superconductors
ArXiv cond-mat/9812155 (1998)
Abstract:
We study a delocalization transition for non-interacting quasiparticles moving in two dimensions, which belongs to a new symmetry class. This symmetry class can be realised in a dirty, gapless superconductor in which time reversal symmetry for orbital motion is broken, but spin rotation symmetry is intact. We find a direct transition between two insulating phases with quantized Hall conductances of zero and two for the conserved quasiparticles. The energy of quasiparticles acts as a relevant, symmetry-breaking field at the critical point, which splits the direct transition into two conventional plateau transitions.Eigenvector statistics in non-hermitian random matrix ensembles
Physical Review Letters 81:16 (1998) 3367-3370
Abstract:
We study statistical properties of the eigenvectors of non-Hermitian random matrices, concentrating on Ginibre’s complex Gaussian ensemble, in which the real and imaginary parts of each element of an N × N matrix, J, are independent random variables. Calculating ensemble averages based on the quantity ⟨Lα|Lβ⟩ ⟨Rβ|Rα⟩, where ⟨Lα| and |Rβ⟩ are left and right eigenvectors of J, we show for large N that eigenvectors associated with a pair of eigenvalues are highly correlated if the two eigenvalues lie close in the complex plane. We examine consequences of these correlations that are likely to be important in physical applications. © 1998 The American Physical Society.The transverse magnetoresistance of the two-dimensional chiral metal
ArXiv cond-mat/9809286 (1998)
Abstract:
We consider the two-dimensional chiral metal, which exists at the surface of a layered, three-dimensional sample exhibiting the integer quantum Hall effect. We calculate its magnetoresistance in response to a component of magnetic field perpendicular to the sample surface, in the low temperature, but macroscopic, regime where inelastic scattering may be neglected. The magnetoresistance is positive, following a Drude form with a field scale, $B_0=\Phi_0/al_{\text{el}}$, given by the transverse field strength at which one quantum of flux, $\Phi_0$, passes through a rectangle with sides set by the layer-spacing, $a$, and the elastic mean free path, $l_{\text{el}}$. Experimental measurement of this magnetoresistance may therefore provide a direct determination of the elastic mean free path in the chiral metal.Eigenvector statistics in non-Hermitian random matrix ensembles
ArXiv cond-mat/9809090 (1998)