396 research outputs found

    Josephson Spin Current in Triplet Superconductor Junctions

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    This paper theoretically discusses the spin current in spin-triplet superconductor / insulator / spin-triplet superconductor junctions. At low temperatures, a midgap Andreev resonant state anomalously enhances not only the charge current but also the spin current. The coupling between the Cooper pairs and the electromagnetic fields leads to the Frounhofer pattern in the direct current spin flow in magnetic fields and the alternative spin current under applied bias-voltages.Comment: 4 pages, 2 figure

    Josephson Effect in Noncentrosymmetric Superconductor Junctions

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    We discuss the Josephson current between two noncentrosymmetric superconductors. The coexistence of superconducting order parameters between spin-singlet ΔS\Delta_{\text{S}} and helical p-wave spin-triplet ΔT\Delta_{\text{T}} enriches a variety of low-temperature behavior of Josephson current depending on their relative amplitudes. We will show that characteristic behaviors of the Josephson current for ΔS>ΔT\Delta_{\text{S}} > \Delta_{\text{T}} are clearly different from those for ΔS<ΔT\Delta_{\text{S}} < \Delta_{\text{T}}. The topologically protected zero-energy surface bound states are responsible for the clear difference. We conclude that the Josephson current well reflects character of the topological surface states and the pairing symmetry of noncentrosymmetric superconductors.Comment: 7 pages, 6 figures embedde

    Three-dimensional symmetry breaking topological matters

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    We discuss topological electronic states described by the Dirac Hamiltonian plus an additional one in three-dimension. When the additional Hamiltonian is an element of an Abelian group, electronic states become topologically nontrivial even in the absence of fundamental symmetries such as the time-reversal and the particle-hole symmety. The symmetry-breaking topological states are charercterized by the Chern number defined in the two-dimensional partial Brillouin zone. The topological insulators under Zeeman field are an example of the symmetry-breaking topological matters. We show the transision from the topological insulating phase to the topological semimetal one under the strong Zeeman field.Comment: 5 pages, 4 figure

    Stability of flat zero-energy states at the dirty surface of a nodal superconductor

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    We discuss the stability of highly degenerate zero-energy states tha appear at the surface of a nodal superconductor preserving time-reversal symmetry. The existence of such surface states is a direct consequence of the nontrivial topological numbers defined in the restricted Brillouin zones in the clean limit. In experiments, however, potential disorder is inevitable near the surface of a real superconductor, which may lift the high degeneracy at zero energy. We show that an index defined in terms of the chiral eigenvalues of the zero-energy states can be used to measure the degree of degeneracy at zero energy in the presence of potential disorder. We also discuss the relationship between the index and the topological numbers.Comment: 12 pages, 7 figure

    Robustness of Gapless Interface State in a Junction of Two Topological Insulators

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    We theoretically study subgap states appearing at the interface between two three-dimensional topological insulators which have different configurations in the spin-orbit interactions from each other. The coupling of spin σ\boldsymbol{\sigma} with momenta p\boldsymbol{p} is configured by a material dependent 3×33\times 3 matrix Λ\boldsymbol{\Lambda} as σμΛμνpν{\sigma}^\mu {\Lambda}_\mu^\nu p_\nu. We show that the spectra of the interface suggap states depend strongly on the relative choices of Λ\boldsymbol{\Lambda} in the two topological insulators. In particular, we focus on properties of gapless states which appear when Λ\boldsymbol{\Lambda} in two topological insulators are connected by the inversion in momentum space. We also discuss the robustness of the gapless states under perturbations breaking the time-reversal symmetry or the band-inversion symmetry by the numerical simulation.Comment: 13 pages, 9 figure

    Effects of surface roughness on the paramagnetic response of small unconventional superconductors

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    We theoretically study effects of surface roughness on the magnetic response of small unconventional superconductors by solving the Eilenberger equation for the quassiclassical Green function and the Maxwell equation for the vector potential simultaneously and self-consistently. The paramagnetic phase of spin-singlet dd-wave superconducting disks is drastically suppressed by the surface roughness, whereas that of spin-triplet pp-wave disks is robust even in the presence of the roughness. Such difference derives from the orbital symmetry of paramagnetic odd-frequency Cooper pairs appearing at the surface of disks. The orbital part of the paramagnetic pairing correlation is pp-wave symmetry in the dd-wave disks, whereas it is ss-wave symmetry in the pp-wave ones. Calculating the free-energy, we also confirm that the paramagnetic state is more stable than the normal state, which indicates a possibility of detecting the paramagnetic effect in experiments. Indeed our results are consistent with an experimental finding on high-TcT_c thin films.Comment: 11 pages, 10 figure

    Green function theory of dirty two-band superconductivity

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    We study the effects of random nonmagnetic impurities on the superconducting transition temperature TcT_c in a two-band superconductor, where we assume the equal-time spin-singlet s-wave pair potential in each conduction band and the hybridization between the two bands as well as the band asymmetry. In the clean limit, the phase of hybridization determines the stability of two states: called s++s_{++} and s+s_{+-}. The interband impurity scatterings decrease TcT_c of the two states exactly in the same manner when the Hamiltonian preserves time-reversal symmetry. We find that a superconductor with larger hybridization shows more moderate suppression of TcT_c. This effect can be explained by the presence of odd-frequency Cooper pairs which are generated by the band hybridization in the clean limit and are broken by impurities.Comment: 11 pages, 2 figure
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