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      Impurity bound states in fully gapped \(d\)-wave superconductors with subdominant order parameters

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          Abstract

          Impurities in superconductors and their induced bound states are important both for engineering novel states such as Majorana zero-energy modes and for probing bulk properties of the superconducting state. The high-temperature cuprates offer a clear advantage in a much larger superconducting order parameter, but the nodal energy spectrum of a pure \(d\)-wave superconductor only allows virtual bound states. Fully gapped \(d\)-wave superconducting states have however been proposed in several cuprate systems thanks to subdominant order parameters producing \(d+is\)- or \(d+id'\)-wave superconducting states. Here we study both magnetic and potential impurities in these fully gapped \(d\)-wave superconductors. Using analytical T-matrix and complementary numerical tight-binding lattice calculations, we show that magnetic and potential impurities behave fundamentally different in \(d+is\)- and \(d+id'\)-wave superconductors. In a \(d+is\)-wave superconductor, there are no bound states for potential impurities, while a magnetic impurity produces one pair of bound states, with a zero-energy level crossing at a finite scattering strength. On the other hand, a \(d+id'\)-wave symmetry always give rise to two pairs of bound states and only produce a reachable zero-energy level crossing if the normal state has a strong particle-hole asymmetry.

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          Signatures of Majorana fermions in hybrid superconductor-semiconductor nanowire devices

          Majorana fermions are particles identical to their own antiparticles. They have been theoretically predicted to exist in topological superconductors. We report electrical measurements on InSb nanowires contacted with one normal (Au) and one superconducting electrode (NbTiN). Gate voltages vary electron density and define a tunnel barrier between normal and superconducting contacts. In the presence of magnetic fields of order 100 mT we observe bound, mid-gap states at zero bias voltage. These bound states remain fixed to zero bias even when magnetic fields and gate voltages are changed over considerable ranges. Our observations support the hypothesis of Majorana fermions in nanowires coupled to superconductors.
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            Observation of Majorana Fermions in Ferromagnetic Atomic Chains on a Superconductor

            Majorana fermions are predicted to localize at the edge of a topological superconductor, a state of matter that can form when a ferromagnetic system is placed in proximity to a conventional superconductor with strong spin-orbit interaction. With the goal of realizing a one-dimensional topological superconductor, we have fabricated ferromagnetic iron (Fe) atomic chains on the surface of superconducting lead (Pb). Using high-resolution spectroscopic imaging techniques, we show that the onset of superconductivity, which gaps the electronic density of states in the bulk of the Fe chains, is accompanied by the appearance of zero energy end states. This spatially resolved signature provides strong evidence, corroborated by other observations, for the formation of a topological phase and edge-bound Majorana fermions in our atomic chains.
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              Impurity-induced states in conventional and unconventional superconductors

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                Author and article information

                Journal
                2016-12-12
                Article
                1612.03619
                985b484c-c914-422b-b430-ef3245e16cc6

                http://arxiv.org/licenses/nonexclusive-distrib/1.0/

                History
                Custom metadata
                10 pages, 6 figures
                cond-mat.supr-con cond-mat.str-el

                Condensed matter
                Condensed matter

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