7,231 research outputs found

    Existence and smoothness of the stable foliation for sectional hyperbolic attractors

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    We prove the existence of a contracting invariant topological foliation in a full neighborhood for partially hyperbolic attractors. Under certain bunching conditions it can then be shown that this stable foliation is smooth. Specialising to sectional hyperbolic attractors, we give a verifiable condition for bunching. In particular, we show that the stable foliation for the classical Lorenz equation (and nearby vector fields) is better than C1C^1 which is crucial for recent results on exponential decay of correlations. In fact the foliation is at least C1.278C^{1.278}.Comment: Corrected estimate for smoothness of stable foliation. Clarification of which results hold for general partially hyperbolic attractors. Some minor typos fixed. Accepted for publication in Bull. London Math. So

    Hall conductivity as bulk signature of topological transitions in superconductors

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    Topological superconductors may undergo transitions between phases with different topological numbers which, like the case of topological insulators, are related to the presence of gapless (Majorana) edge states. In Z\mathbb{Z} topological insulators the charge Hall conductivity is quantized, being proportional to the number of gapless states running at the edge. In a superconductor, however, charge is not conserved and, therefore, σxy\sigma_{xy} is not quantized, even in the case of a Z\mathbb{Z} topological superconductor. Here it is shown that while the σxy\sigma_{xy} evolves continuously between different topological phases of a Z\mathbb{Z} topological superconductor, its derivatives display sharp features signaling the topological transitions. We consider in detail the case of a triplet superconductor with p-wave symmetry in the presence of Rashba spin-orbit (SO) coupling and externally applied Zeeman spin splitting. Generalization to the cases where the pairing vector is not aligned with that of the SO coupling is given. We generalize also to the cases where the normal system is already topologically non-trivial.Comment: 10 pages, 10 figure
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