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      Superconductivity Reinforced by Magnetic Field and the Magnetic Instability in Uranium Ferromagnets

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          Superconductivity on the border of itinerant-electron ferromagnetism in UGe2

          The absence of simple examples of superconductivity adjoining itinerant-electron ferromagnetism in the phase diagram has for many years cast doubt on the validity of conventional models of magnetically mediated superconductivity. On closer examination, however, very few systems have been studied in the extreme conditions of purity, proximity to the ferromagnetic state and very low temperatures required to test the theory definitively. Here we report the observation of superconductivity on the border of ferromagnetism in a pure system, UGe2, which is known to be qualitatively similar to the classic d-electron ferromagnets. The superconductivity that we observe below 1 K, in a limited pressure range on the border of ferromagnetism, seems to arise from the same electrons that produce band magnetism. In this case, superconductivity is most naturally understood in terms of magnetic as opposed to lattice interactions, and by a spin-triplet rather than the spin-singlet pairing normally associated with nearly antiferromagnetic metals.
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            Coexistence of superconductivity and ferromagnetism in URhGe.

            The discovery of superconductivity at high pressure (albeit over a restricted range) in the ferromagnetic material UGe2 raised the possibility that bulk superconductivity might be found in other ferromagnets. The exact symmetry of the paired state and the dominant mechanism responsible for the pairing, however, remain unidentified. Meanwhile, the conjecture that superconductivity could occur more generally in ferromagnets has been fuelled by the recent observation of a low-temperature transition that suggests an onset of superconductivity in high-quality crystals of the itinerant-ferromagnet ZrZn2 (ref. 2), although the thermodynamic signature of this transition could not be detected. Here we show that the ferromagnet URhGe is superconducting at ambient pressure. In this case, we find the thermodynamic signature of the transition-its form is consistent with a superconducting pairing of a spin-triplet type, although further testing with cleaner samples is needed to confirm this. The combination of superconductivity and ferromagnetism may thus be more common and consequently more important than hitherto realized.
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              Coexistence ofp-state superconductivity and itinerant ferromagnetism

              D Fay, J. Appel (1980)
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                Author and article information

                Journal
                Journal of the Physical Society of Japan
                J. Phys. Soc. Jpn.
                Japan Society of Applied Physics
                0031-9015
                1347-4073
                January 02 2011
                January 02 2011
                : 80
                : Suppl.A
                : SA008
                Affiliations
                [1 ]INAC/SPSMS, CEA-Grenoble, 17 rue des Martyrs, 38054 Grenoble, France
                [2 ]Advanced Science Research Center, Japan Atomic Energy Agency, Tokai, Ibaraki 319-1195, Japan
                [3 ]KIT-Karlsruhe, Institut für Festkörperphysik, 76021 Karlsruhe, Germany
                [4 ]LNCMI-G, CNRS, 25 rue des Martyrs, 38042 Grenoble, France
                [5 ]Institut Néel, CNRS, 25 rue des Martyrs, 38042 Grenoble, France
                Article
                10.1143/JPSJS.80SA.SA008
                6694c22c-c6b0-4620-83c5-fa646775b452
                © 2011
                History

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