8,888 research outputs found

    Gap Symmetry an Thermal Conductivity in Nodal Superconductors

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    There are now many nodal superconductors in heavy fermion (HF) systems, charge conjugated organic metals, high Tc cuprates and ruthenates. On the other hand only few of them have a well established gap function. We present here a study of the angular dependent thermal conductivity in the vortex state of some of the nodal superconductors. We hope it will help to identify the nodal directions in the gap function of UPd_2Al_3, UNi_2Al_3, UBe_13 and URu_2Si_2.Comment: 4 pages, 5 figure

    Nonlinear response and scaling law in the vortex state of d-wave superconductors

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    We study the field dependence of the quasi-particle density of states, the thermodynamics and the transport properties in the vortex state of d-wave superconductors when a magnetic field is applied perpendicular to the conducting plane, specially for the low field and the low temperature compared to the upper critical field and transition temperature, respectively, H/Hc21H/H_{c2} \ll 1 and T/Tc1T/T_c \ll 1. Both the superfluid density and the spin susceptibility exhibit the characteristic H\sqrt{H}-field dependence, while the nuclear spin lattice relaxation rate T11_1^{-1} and the thermal conductivity are linear in field HH. With increasing temperature, these quantities exhibit the scaling behavior in T/HT/\sqrt{H}. The present theory applies to 2D ff-wave superconductor as well; a possible candidate of the superconductivity in Sr2_2RuO4_4.Comment: 11 pages, 4 figure

    Gap Symmetry of Superconductivity in UPd2Al3

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    The angle dependent thermal conductivity of the heavy-fermion superconductor UPd2_2Al3_3 in the vortex state was recently measured by Watanabe et al. Here we analyze this data from two perspectives: universal heat conduction and the angle-dependence. We conclude that the superconducting gap function Δ(k)\Delta({\bf k}) in UPd2_2Al3_3 has horizontal nodes and is given by Δ(k)=Δcos(2χ)\Delta({\bf k}) =\Delta\cos(2\chi), with χ=ckz\chi = ck_{z}.Comment: 8 pages, 4 figures, improved figures in replacemen

    Novel vortex lattice transition in d-wave superconductors

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    We study the vortex state in a magnetic field parallel to the cc axis in the framework of the extended Ginzburg Landau equation. We find the vortex acquires a fourfold modulation proportional to cos(4ϕ)\cos(4\phi) where ϕ\phi is the angle r{\bf r} makes with the aa-axis. This term gives rise to an attractive interaction between two vortices when they are aligned parallel to (1,1,0)(1,1,0) or (1,1,0)(1,-1,0). We predict the first order vortex lattice transition at B=Hcrκ1Hc2(t)B=H_{cr}\sim \kappa^{-1} H_{c2}(t) from triangular into the square lattice tilted by 4545^\circ from the aa axis. This gives the critical field HcrH_{cr} a few Tesla for YBCO and Bi2212 monocrystals at low temperatures (T10KT\leq 10 K).Comment: 6 pages, 4 figure

    Gap Structure of the Spin-Triplet Superconductor Sr2RuO4 Determined from the Field-Orientation Dependence of Specific Heat

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    We report the field-orientation dependent specific heat of the spin-triplet superconductor Sr2RuO4 under the magnetic field aligned parallel to the RuO2 planes with high accuracy. Below about 0.3 K, striking 4-fold oscillations of the density of states reflecting the superconducting gap structure have been resolved for the first time. We also obtained strong evidence of multi-band superconductivity and concluded that the superconducting gap in the active band, responsible for the superconducting instability, is modulated with a minimum along the [100] direction.Comment: 4 pages, 4 figure

    Low-lying excitations around a single vortex in a d-wave superconductor

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    A full quantum-mechanical treatment of the Bogoliubov-de Gennes equation for a single vortex in a d-wave superconductor is presented. First, we find low-energy states extended in four diagonal directions, which have no counterpart in a vortex of s-wave superconductors. The four-fold symmetry is due to 'quantum effect', which is enhanced when pFξp_{F}\xi is small. Second, for pFξ1p_{F}\xi \sim 1, a peak with a large energy gap E0ΔE_{0}\sim \Delta is found in the density of states, which is due to the formation of the lowest bound states.Comment: 7pages, Revte

    Thermal conductivity in B- and C- phase of UPt_3

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    Although the superconductivity in UPt_3 is one of the most well studied, there are still lingering questions about the nodal directions in the B and C phase in the presence of a magnetic field. Limiting ourselves to the low temperature regime (T<<Delta(0)), we study the magnetothermal conductivity with in semiclassical approximation using Volovik's approach. The angular dependence of the magnetothermal conductivity for an arbitrary field direction should clarify the nodal structure in UPt_3.Comment: 4 pages, 5 figure

    Laboratory evaluation of a rapid IgG4 antibody test (BLF Rapid™) for bancroftian filariasis

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    At the end phase of the Global Programme to Eliminate Lymphatic Filariasis, antibody testing may have a role in decision-making for bancroftian filariasis–endemic areas. This study evaluated the diagnostic performance of BLF Rapid ™ , a prototype immunochromatographic IgG4-based test using BmSXP recombinant protein, for detection of bancroftian filariasis. The test was evaluated using 258 serum samples, comprising 96 samples tested at Universiti Sains Malaysia (in-house) and 162 samples tested independently at three international laboratories in the USA and India, and two laboratories in Malaysia. The independent testing involved 99 samples from Wuchereria bancrofti microfilaria or antigen positive individuals and 63 samples from people who were healthy or had other infections. The in-house evaluation showed 100% diagnostic sensitivity and specificity. The independent evaluations showed a diagnostic sensitivity of 84–100% and 100% specificity (excluding non-lymphatic filarial infections). BLF Rapid has potential as a surveillance diagnostic tool to make “Transmission Assessment Survey”–stopping decisions and conduct post-elimination surveillance

    Magnetization reversal in Kagome artificial spin ice studied by first-order reversal curves

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    Magnetization reversal of interconnected Kagome artificial spin ice was studied by the first-order reversal curve (FORC) technique based on the magneto-optical Kerr effect and magnetoresistance measurements. The magnetization reversal exhibits a distinct six-fold symmetry with the external field orientation. When the field is parallel to one of the nano-bar branches, the domain nucleation/propagation and annihilation processes sensitively depend on the field cycling history and the maximum field applied. When the field is nearly perpendicular to one of the branches, the FORC measurement reveals the magnetic interaction between the Dirac strings and orthogonal branches during the magnetization reversal process. Our results demonstrate that the FORC approach provides a comprehensive framework for understanding the magnetic interaction in the magnetization reversal processes of spin-frustrated systems
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