349 research outputs found

    Microwave Penetration Depth and Quasiparticle Conductivity in PrFeAsO_1-y Single Crystals : Evidence for a Full-Gap Superconductor

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    In-plane microwave penetration depth λab\lambda_{ab} and quaiparticle conductivity at 28 GHz are measured in underdoped single crystals of the Fe-based superconductor PrFeAsO1y_{1-y} (Tc35T_c\approx 35 K) by using a sensitive superconducting cavity resonator. λab(T)\lambda_{ab}(T) shows flat dependence at low temperatures, which is incompatible with the presence of nodes in the superconducting gap Δ(k)\Delta({\bf k}). The temperature dependence of the superfluid density demonstrates that the gap is non-zero (Δ/kBTc1.6\Delta/k_BT_c\gtrsim 1.6) all over the Fermi surface. The microwave conductivity below TcT_c exhibits an enhancement larger than the coherence peak, reminiscent of high-TcT_c cuprate superconductors.Comment: 4 pages, 3 figures. Version accepted for publication in Phys. Rev. Lett. For related results of hole-doped 122 system, see arXiv:0810.350

    Microwave Surface-Impedance Measurements of the Magnetic Penetration Depth in Single Crystal Ba1-xKxFe2As2 Superconductors: Evidence for a Disorder-Dependent Superfluid Density

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    We report high-sensitivity microwave measurements of the in-plane penetration depth λab\lambda_{ab} and quasiparticle scattering rate 1/τ1/\tau in several single crystals of hole-doped Fe-based superconductor Ba1x_{1-x}Kx_xFe2_2As2_2 (x0.55x\approx 0.55). While power-law temperature dependence of λab\lambda_{ab} with the power 2\sim 2 is found in crystals with large 1/τ1/\tau, we observe exponential temperature dependence of superfluid density consistent with the existence of fully opened two gaps in the cleanest crystal we studied. The difference may be a consequence of different level of disorder inherent in the crystals. We also find a linear relation between the low-temperature scattering rate and the density of quasiparticles, which shows a clear contrast to the case of d-wave cuprate superconductors with nodes in the gap. These results demonstrate intrinsically nodeless order parameters in the Fe-arsenides.Comment: 4 pages, 4 figures, 1 table. Accepted for publication in Phys. Rev. Lett. Changed title as suggested by the PRL editor

    Line nodes in the energy gap of high-temperature superconducting BaFe_2(As_{1-x}P_x)_2 from penetration depth and thermal conductivity measurements

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    We report magnetic penetration depth and thermal conductivity data for high-quality single crystals of BaFe2_2(As1x_{1-x}Px_{x})2_2 (Tc=30T_c=30\,K) which provide strong evidence that this material has line nodes in its energy gap. This is distinctly different from the nodeless gap found for (Ba,K)Fe2_2As2_2 which has similar TcT_c and phase diagram. Our results indicate that repulsive electronic interactions play an essential role for Fe-based high-TcT_c superconductivity but that uniquely there are distinctly different pairing states, with and without nodes, which have comparable TcT_c.Comment: 4 pages, 3 figures, revised version to be published in Phys. Rev. B Rapid Communicatio

    Superconducting Gap Structure of LaFePO Studied by Thermal Conductivity

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    The superconducting gap structure of LaFePO (Tc=7.4T_c=7.4 K) is studied by thermal conductivity (κ\kappa) at low temperatures in fields HH parallel and perpendicular to the c axis. A clear two-step field dependence of κ(H)\kappa(H) with a characteristic field Hs(350H_s(\sim 350 Oe) much lower than the upper critical field Hc2H_{c2} is observed. In spite of large anisotropy of Hc2H_{c2}, κ(H)\kappa(H) in both HH-directions is nearly identical below HsH_s. Above HsH_s, κ(H)\kappa(H) grows gradually with HH with a convex curvature, followed by a steep increase with strong upward curvature near Hc2H_{c2}. These results indicate the multigap superconductivity with active two-dimensional (2D) and passive 3D bands having contrasting gap values. Together with the recent penetration depth results, we suggest that the 2D bands consist of nodal and nodeless ones, consistent with the extended s-wave symmetry

    Structural properties and superconductivity of SrFe2As2-xPx and CaFe2As2-yPy

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    The SrFe2As2-xPx and CaFe2As2-yPy materials were prepared by a solid state reaction method. X-ray diffraction measurements indicate the single-phase samples can be successfully obtained for SrFe2As2-xPx and CaFe2As2-yPy samples. Clear contraction of the lattice parameters are clearly determined due to the relatively smaller P ions substation for As. The SDW instability associated with tetragonal to orthorhombic phase transition is suppressed visibly in both systems following with the increase of P contents. The highest superconducting transitions are respectively observed at about 27 K in SrFe2As1.3P0.7 and at about 13 K in CaFe2As1.7P0.3.Comment: 11 pages, 5 figures, 2 table

    Structural reorganization of cylindrical nanoparticles triggered by polylactide stereocomplexation

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    YesCo-crystallization of polymers with different configurations/tacticities provides access to materials with enhanced performance. The stereocomplexation of isotactic poly(L-lactide) and poly(D-lactide) has led to improved properties compared with each homochiral material. Herein, we report the preparation of stereocomplex micelles from a mixture of poly(L-lactide)-b-poly(acrylic acid) and poly(D-lactide)-b-poly(acrylic acid) diblock copolymers in water via crystallization-driven self-assembly. During the formation of these stereocomplex micelles, an unexpected morphological transition results in the formation of dense crystalline spherical micelles rather than cylinders. Furthermore, mixture of cylinders with opposite homochirality in either THF/H2O mixtures or in pure water at 65 °C leads to disassembly into stereocomplexed spherical micelles. Similarly, a transition is also observed in a related PEO-b-PLLA/PEO-b-PDLA system, demonstrating wider applicability. This new mechanism for morphological reorganization, through competitive crystallization and stereocomplexation and without the requirement for an external stimulus, allows for new opportunities in controlled release and delivery applications.University of Warwick, Swiss National Science Foundation and the EPSRC. The Royal Society - an Industry Fellowship to A.P.D. The Engineering and Physical Sciences Research Council (EP/G004897/1) - funding to support postdoctoral fellowships for A.P.B. as well as funding for J.S. and M.A.D. through the Warwick Centre for Analytical Science (EP/F034210/1). The Science City Research Alliance and the HEFCE Strategic Development Fund - funding support. Some items of equipment that were used in this research were funded by Birmingham Science City, with support from Advantage West Midlands and part-funded by the European Regional Development Fund
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