366 research outputs found

    Evolution of Paramagnetic Quasiparticle Excitations Emerged in the High-Field Superconducting Phase of CeCoIn5

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    We present In NMR measurements in a novel thermodynamic phase of CeCoIn5 in high magnetic field, where exotic superconductivity coexists with the incommensurate spin-density wave order. We show that the NMR spectra in this phase provide direct evidence for the emergence of the spatially distributed normal quasiparticle regions. The quantitative analysis for the field evolution of the paramagnetic magnetization and newly-emerged low-energy quasiparticle density of states is consistent with the nodal plane formation, which is characterized by an order parameter in the Fulde-Ferrell-Larkin-Ovchinnikov (FFLO) state. The NMR spectra also suggest that the spatially uniform spin-density wave is induced in the FFLO phase.Comment: 4 pages, 4 figures, accepted for publication in Phys. Rev. Let

    Quantum critical point lying beneath the superconducting dome in iron-pnictides

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    Whether a quantum critical point (QCP) lies beneath the superconducting dome has been a long-standing issue that remains unresolved in many classes of unconventional superconductors, notably cuprates, heavy fermion compounds and most recently iron-pnictides. The existence of a QCP may offer a route to understand: the origin of their anomalous non-Fermi liquid properties, the microscopic coexistence between unconventional superconductivity and magnetic or some exotic order, and ultimately the mechanism of superconductivity itself. The isovalent substituted iron-pnictide BaFe2_2(As1x_{1-x}Px_x)2_2 offers a new platform for the study of quantum criticality, providing a unique opportunity to study the evolution of the electronic properties in a wide range of the phase diagram. Recent experiments in BaFe2_2(As1x_{1-x}Px_x)2_2 have provided the first clear and unambiguous evidence of a second order quantum phase transition lying beneath the superconducting dome.Comment: 15 pages, 6 figures, review article submitted to Annual Review of Condensed Matter Physic

    Unconventional superconductivity and antiferromagnetic quantum critical behavior in the isovalent-doped BaFe2(As1-xPx)2

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    Spin dynamics evolution of BaFe2_2(As1x_{1-x}Px_x)2_2 was probed as a function of P concentration via 31^{31}P NMR. Our NMR study reveals that two-dimensional antiferromagnetic (AF) fluctuations are notably enhanced with little change in static susceptibility on approaching the AF phase from the superconducting dome. Moreover, magnetically ordered temperature θ\theta deduced from the relaxation rate vanishes at optimal doping. These results provide clear-cut evidence for a quantum-critical point (QCP), suggesting that the AF fluctuations associated with the QCP play a central role in the high-TcT_c superconductivity.Comment: 5 pages, 3 figure

    Surface impedance anisotropy of YBa2_2Cu3_3O6.95_{6.95} single crystals: electrodynamic basis of the measurements

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    An electrodynamic technique is developed for determining the components of surface impedance and complex conductivity tensors of HTSC single crystals on the basis of measured quantities of a quality factor and a resonator frequency shift. A simple formula is obtained for a geometrical factor of a crystal in the form of a plate with dimensions ba>cb\gg a>c in a microwave magnetic field Hωab{\bf H_{\omega}}\perp ab. To obtain the c-axis complex conductivity from measurements at Hωab{\bf H_{\omega}}\parallel ab we propose a procedure which takes account of sample size effects. With the aid of the technique involved temperature dependences of all impedance and conductivity tensors components of YBa2_2Cu3_3O6.95_{6.95} single crystal, grown in BaZrO3_3 crucible, are determined at a frequency of f=9.4f=9.4 GHz in its normal and superconducting states. All of them proved to be linear at T<Tc/2T<T_c/2, and their extrapolation to zero temperature gives the values of residual surface resistance Rab(0)40R_{ab}(0)\approx 40 μΩ\mu\Omega and Rc(0)0.8R_c(0)\approx 0.8 mΩ\Omega and magnetic field penetration depth λab(0)150\lambda_{ab}(0)\approx 150 nm and λc(0)1.55\lambda_c(0)\approx 1.55 μ\mum.Comment: 9 pages, 7 figures. Submitted to Phys.Rev.B 05Jun2002; accepted for publication 21Febr200
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