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      Symmetry protected line nodes in non-symmorphic magnetic space groups: Applications to UCoGe and UPd\(_2\)Al\(_3\)

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          Abstract

          We present the group-thoretical classification of gap functions in superconductors coexisting with some magnetic order in non-symmorphic magnetic space groups. Based on the weak-coupling BCS theory, we show that UCoGe-type ferromagnetic superconductors must have horizontal line nodes on either \(k_z=0\) or \(\pm\pi/c\) plane. Moreover, it is likely that additional Weyl point nodes exist at the axial point. On the other hand, in UPd\(_2\)Al\(_3\)-type antiferromagnetic superconductors, gap functions with \(A_g\) symmetry possess horizontal line nodes in antiferromagnetic Brillouin zone boundary perpendicular to \(c\)-axis. In other words, the conventional fully-gapped \(s\)-wave superconductivity is forbidden in this type of antiferromagnetic superconductors, irrelevant to the pairing mechanism, as long as the Fermi surface crosses a zone boundary. UCoGe and UPd\(_2\)Al\(_3\) are candidates for unconventional superconductors possessing hidden symmetry-protected line nodes, peculiar to non-symmorphic magnetic space groups.

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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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              Order parameter symmetry in ferromagnetic superconductors

              We analyze the symmetry and the nodal structure of the superconducting order parameter in a cubic ferromagnet, such as ZrZn\(_2\). We demonstrate how the order parameter symmetry evolves when the electromagnetic interaction of the conduction electrons with the internal magnetic induction and the spin-orbit coupling are taken into account. These interactions break the cubic symmetry and lift the degeneracy of the order parameter. It is shown that the order parameter which appears immediately below the critical temperature has two components, and its symmetry is described by {\em co-representations} of the magnetic point groups. This allows us to make predictions about the location of the gap nodes.
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                Author and article information

                Journal
                2016-10-14
                Article
                1610.04679
                c19e6572-c9ec-4ba4-a99a-d4b165b2c2d5

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

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                Custom metadata
                7 pages, 2 figures
                cond-mat.supr-con

                Condensed matter
                Condensed matter

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