541 research outputs found

    Specific heat at the transition in a superconductor with fluctuating magnetic moments

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    In the heavy-fermion materials CeCoIn5_5 and UBe13_{13}, the superconducting order parameter is coupled to flucutating magnetization of the uncompensated part of the localized ff-moments. We find that this coupling decreases the superconducting transition temperature and increases the jump of the specific-heat coefficient, which indicates entropy transfer from the magnetic to the superconducting degree of freedom at the transition temperature. Below the transition, we find that the magnetic fluctuations are suppressed. We discuss the relation of our results to experiments on CeCoIn5_5 under pressure.Comment: 4 pages, 1 figur

    Local edge modes in doped cuprates with checkerboard polaronic heterogeneity

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    We study a periodic polaronic system, which exhibits a nanoscale superlattice structure, as a model for hole-doped cuprates with checkerboard-like heterogeneity, as has been observed recently by scanning tunneling microscopy (STM). Within this model, the electronic and phononic excitations are investigated by applying an unrestricted Hartree-Fock and a random phase approximation (RPA) to a multiband Peierls-Hubbard Hamiltonian in two dimensions

    Uncovering the Hidden Order in URu2Si2 by Impurity Doping

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    We report the use of impurities to probe the hidden order parameter of the strongly correlated metal URu_2Si_2 below the transition temperature T_0 ~ 17.5 K. The nature of this order parameter has eluded researchers for more than two decades, but is accompanied by the development of a partial gap in the single particle density of states that can be detected through measurements of the electronic specific heat and nuclear spin-lattice relaxation rate. We find that impurities in the hidden order phase give rise to local patches of antiferromagnetism. An analysis of the coupling between the antiferromagnetism and the hidden order reveals that the former is not a competing order parameter but rather a parasitic effect of the latter.Comment: 4 pages, 4 figure

    NMR investigation of the Knight shift anomaly in CeIrIn5 at high magnetic fields

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    We report nuclear magnetic resonance Knight shift data in the heavy fermion material CeIrIn5 at fields up to 30 T. The Knight shift of the In displays a strong anomaly, and we analyze the results using two different interpretations. We find that the Kondo lattice coherence temperature and the effective mass of the heavy electrons remains largely unaffected by the magnetic field, despite the fact that the Zeeman energy is on the order of the coherence temperature.Comment: 5 pages, 5 figures; to appear in Phys. Rev.

    Hybridization-driven gap in U3Bi4Ni3: a 209Bi NMR/NQR study

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    We report 209Bi NMR and NQR measurements on a single crystal of the Kondo insulator U3Bi4Ni3. The 209Bi nuclear spin-lattice relaxation rate (T11T_1^{-1}) shows activated behavior and is well-fit by a spin gap of 220 K. The 209Bi Knight shift (K) exhibits a strong temperature dependence arising from 5f electrons, in which K is negative at high temperatures and increases as the temperature is lowered. Below 50 K, K shows a broad maximum and decreases slightly upon further cooling. Our data provide insight into the evolution of the hyperfine fields in a fully gapped Kondo insulator based on 5f electron hybridization.Comment: 4 pages, 4 figures, submitted to Phys. Rev.

    Cluster Spin Glass Distribution Functions in La2x_{2-x}Srx_xCuO4_4

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    Signatures of the cluster spin glass have been found in a variety of experiments, with an effective onset temperature TonT_{on} that is frequency dependent. We reanalyze the experimental results and find that they are characterized by a distribution of activation energies, with a nonzero glass transition temperature Tg(x)<TonT_g(x)<T_{on}. While the distribution of activation energies is the same, the distribution of weights depends on the process. Remarkably, the weights are essentially doping independent.Comment: 5 pages, 5 ps figure

    Local Magnetic Inhomogeneities in Lightly Doped BaFe2_2As2_2

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    We report 75^{75}As NMR measurements in BaFe2_2As2_2 doped with Ni. Like Co, Ni doping suppresses the antiferromagnetic and structural phase transitions and gives rise to superconductivity for sufficiently large Ni doping. The spin lattice relaxation rate diverges at TNT_N, with a critical exponent consistent with 3D ordering of local moments. In the ordered state the spectra quickly broaden inhomogeneously with doping. We extract the average size of the ordered moment as a function of doping, and show that a model in which the order remains commensurate but with local amplitude variations in the vicinity of the dopant fully explains our observations.Comment: 4 pages, 4 figure

    Stripes Disorder and Correlation lengths in doped antiferromagnets

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    For stripes in doped antiferromagnets, we find that the ratio of spin and charge correlation lenghts, ξs/ξc\xi_{s}/\xi_{c}, provide a sharp criterion for determining the dominant form of disorder in the system. If stripes disorder is controlled by topological defects then ξs/ξc1\xi_{s}/\xi_{c}\lesssim 1. In contast, if stripes correlations are disordered primarily by non-topological elastic deformations (i.e., a Bragg-Glass type of disorder) then 1<ξs/ξc41<\xi _{s}/\xi_{c}\lesssim 4 is expected. Therefore, the observation of ξs/ξc4\xi _{s}/\xi_{c}\approx 4 in (LaNd)2xSrxCuO4(LaNd)_{2-x}Sr_{x}CuO_{4} and ξs/ξc3\xi_{s}/\xi _{c}\approx 3 in La2/3Sr1/3NiO4La_{2/3}Sr_{1/3}NiO_{4} invariably implies that the stripes are in a Bragg glass type state, and topological defects are much less relevant than commonly assumed. Expected spectral properties are discussed. Thus, we establish the basis for any theoretical analysis of the experimentally obsereved glassy state in these material.Comment: 4 pages, 2 figure

    Disorder in a Quantum Critical Superconductor

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    In four classes of materials, the layered copper-oxides, organics, iron-pnictides and heavy-fermion compounds, an unconventional superconducting state emerges as a magnetic transition is tuned toward absolute zero temperature, that is, toward a magnetic quantum-critical point (QCP). In most materials, the QCP is accessed by chemical substitutions or applied pressure. CeCoIn5 is one of the few materials that are born as a quantum-critical superconductor and, therefore, offers the opportunity to explore the consequences of chemical disorder. Cadmium-doped crystals of CeCoIn5 are a particularly interesting case where Cd substitution induces long-range magnetic order, as in Zn-doped copper-oxides. Applied pressure globally supresses the Cd-induced magnetic order and restores bulk superconductivity. Here we show, however, that local magnetic correlations, whose spatial extent decreases with applied pressure, persist at the extrapolated QCP. The residual droplets of impurity-induced magnetic moments prevent the reappearance of conventional signatures of quantum criticality, but induce a heterogeneous electronic state. These discoveries show that spin droplets can be a source of electronic heterogeneity in classes of strongly correlated electron systems and emphasize the need for caution when interpreting the effects of tuning a correlated system by chemical substitution.Comment: main text and supplementary informatio
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