275 research outputs found

    Dependence of transport coefficients of Yb(Rh1−x_{1-x}Cox_x)2_2Si2_2 intermetallics on temperature and cobalt concentration

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    Dependence of transport coefficients of the Yb(Rh1−x_{1-x}Cox_x)2_2Si2_2 series of alloys on temperature and cobalt concentration is explained by an asymmetric Anderson model which takes into account the exchange scattering of conduction electrons on ytterbium ions and the splitting of 4ff-states by the crystalline electric field (CEF). The substitution of rhodium by cobalt is described as an increase of chemical pressure which reduces the exchange coupling and the CEF splitting. The scaling analysis and numerical NCA solution of the model show that the effective degeneracy of the 4ff-state at a given temperature depends on the relative magnitude of the Kondo scale and the CEF splitting. Thus, we find that dependence of the thermopower, S(T)S(T), on temperature and cobalt concentration can be understood as an interplay of quantum fluctuations, driven by the Kondo effect, and thermal fluctuations, which favor a uniform occupation of the CEF states. The theoretical model captures all the qualitative features of the experimental data and it explains the evolution of the shape of S(T)S(T) with the increase of cobalt concentration.Comment: 8 pages, 4 figure

    Multidimensional entropy landscape of quantum criticality

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    The Third Law of Thermodynamics states that the entropy of any system in equilibrium has to vanish at absolute zero temperature. At nonzero temperatures, on the other hand, matter is expected to accumulate entropy near a quantum critical point (QCP), where it undergoes a continuous transition from one ground state to another. Here, we determine, based on general thermodynamic principles, the spatial-dimensional profile of the entropy S near a QCP and its steepest descent in the corresponding multidimensional stress space. We demonstrate this approach for the canonical quantum critical compound CeCu6-xAux near its onset of antiferromagnetic order. We are able to link the directional stress dependence of S to the previously determined geometry of quantum critical fluctuations. Our demonstration of the multidimensional entropy landscape provides the foundation to understand how quantum criticality nucleates novel phases such as high-temperature superconductivity.Comment: 14 pages, 4 figure

    High-temperature signatures of quantum criticality in heavy fermion systems

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    We propose a new criterion for distinguishing the Hertz-Millis (HM) and the local quantum critical (LQC) mechanism in heavy fermion systems with a magnetic quantum phase transition (QPT). The criterion is based on our finding that the spin screening of Kondo ions can be completely suppressed by the RKKY coupling to the surrounding magnetic ions even without magnetic ordering and that, consequently, the signature of this suppression can be observed in spectroscopic measurements above the magnetic ordering temperature. We apply the criterion to high-resolution photoemission (UPS) measurements on CeCu6−x_{6-x}Aux_{x} and conclude that the QPT in this system is dominated by the LQC scenario.Comment: Inveted paper, International Conference on Magnetism, ICM 2009, Karlsruhe. Published version, added discussions of the relevance of Fermi-surface fluctuations and of a structural transition near the QC

    Anomalous Microwave Surface Resistance of CeCu6

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    We present surface resistance measurements of the archetypical heavy-fermion compound CeCu6 for frequencies between 3.7 and 18 GHz and temperatures from 1.2 to 6 K. The measurements were performed with superconducting stripline resonators that allow simultaneous measurements at multiple frequencies. The surface resistance of CeCu6 exhibits a pronounced decrease below 3 K, in consistence with dc resistivity. The low-temperature frequency dependence of the surface resistance follows a power law with exponent 2/3. While for conventional metals this would be consistent with the anomalous skin effect, we discuss the present situation of a heavy-fermion metal, where this frequency dependence might instead stem from the influence of electronic correlations.Comment: 6 pages, 3 figures, proceedings of SCES 201

    Echo of the Quantum Phase Transition of CeCu6−x_{6-x}Aux_x in XPS: Breakdown of Kondo Screening

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    We present an X-ray photoemission study of the heavy-fermion system CeCu6−x_{6-x}Aux_x across the magnetic quantum phase transition of this compound at temperatures above the single-ion Kondo temperature TKT_K. In dependence of the Au concentration xx we observe a sudden change of the ff-occupation number nfn_f and the core-hole potential UdfU_{df} at the critical concentration xc=0.1x_c=0.1. We interpret these findings in the framework of the single-impurity Anderson model. Our results are in excellent agreement with findings from earlier UPS measurements %\cite{klein08qpt} and provide further information about the precursors of quantum criticality at elevated temperatures.Comment: 5 pages, 3 figures; published version, references updated, minor changes in wordin

    Signature of frustrated moments in quantum critical CePd1−x_{1-x}Nix_xAl

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    CePdAl with Ce 4f4f moments forming a distorted kagom\'e network is one of the scarce materials exhibiting Kondo physics and magnetic frustration simultaneously. As a result, antiferromagnetic (AF) order setting in at TN=2.7T_{\mathrm{N}} = 2.7~K encompasses only two thirds of the Ce moments. We report measurements of the specific heat, CC, and the magnetic Gr\"uneisen parameter, Γmag\Gamma_{\rm mag}, on single crystals of CePd1−x_{1-x}Nix_xAl with x≤0.16x\leq 0.16 at temperatures down to 0.05~K and magnetic fields BB up to 88~T. Field-induced quantum criticality for various concentrations is observed with the critical field decreasing to zero at xc≈0.15x_c\approx 0.15. Remarkably, two-dimensional (2D) AF quantum criticality of Hertz-Millis-Moriya type arises for x=0.05x=0.05 and x=0.1x=0.1 at the suppression of 3D magnetic order. Furthermore, Γmag(B)\Gamma_{\rm mag}(B) shows an additional contribution near 2.52.5~T for all concentrations which is ascribed to correlations of the frustrated one third of Ce moments.Comment: 5+2 pages with 4+3 figure
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