19,034 research outputs found

    Evidence for a quantum phase transition in electron-doped Pr2−x_{2-x}Cex_{x}CuO4−δ_{4-\delta} from Thermopower measurements

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    The evidence for a quantum phase transition under the superconducting dome in the high-TcT_c cuprates has been controversial. We report low temperature normal state thermopower(S) measurements in electron-doped Pr2−x_{2-x}Cex_{x}CuO4−δ_{4-\delta} as a function of doping (x from 0.11 to 0.19). We find that at 2K both S and S/T increase dramatically from x=0.11 to 0.16 and then saturate in the overdoped region. This behavior has a remarkable similarity to previous Hall effect results in Pr2−x_{2-x}Cex_{x}CuO4−δ_{4-\delta} . Our results are further evidence for an antiferromagnetic to paramagnetic quantum phase transition in electron-doped cuprates near x=0.16.Comment: 4 pages, 5 figure

    Comment on "Spectroscopic Evidence for Multiple Order Parameter Components in the Heavy Fermion Superconductor CeCoIn5_5"

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    Recently, Rourke et al. reported point-contact spectroscopy results on the heavy-fermion superconductor CeCoIn5_5 [1]. They obtained conductance spectra on the c-axis surfaces of CeCoIn5_5 single crystals. Their major claims are two-fold: CeCoIn5_5 has i) d-wave pairing symmetry and ii) two coexisting order parameter components. In this Comment, we show that these claims are not warranted by the data presented. [1] Rourke et al., Phys. Rev. Lett. 94, 107005 (2005).Comment: accepted for publication in Phys. Rev. Lett., final for

    Point-contact spectroscopy in heavy-fermion superconductors

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    We develop a minimal model to calculate point-contact spectra between a metallic tip and a superconducting heavy-fermion system. We apply our tunneling model to the heavy fermion CeCoIn5, both in the normal and superconducting state. In point-contact and scanning tunneling spectroscopy many heavy-fermion materials, like CeCoIn5, exhibit an asymmetric differential conductance, dI/dV, combined with a strongly suppressed Andreev reflection signal in the superconducting state. We argue that both features may be explained in terms of a multichannel tunneling model in the presence of localized states near the interface. We find that it is not sufficient to tunnel into two itinerant bands of light and heavy electrons to explain the Fano line shape of the differential conductance. Localized states in the bulk or near the interface are an essential component for quantum interference to occur when an electron tunnels from the metallic tip of the point contact into the heavy-fermion system.Comment: 13 pages, 9 figures. Accepted for publication in Physical Review

    Evidence for Antiferromagnetic Order in La2−x_{2-x}Cex_{x}CuO4_{4} from Angular Magnetoresistance Measurements

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    We investigated the in-plane angular magnetoresistivity (AMR) of T′% T^{^{\prime}}-phase La2−x_{2-x}Cex_{x}CuO4_{4} (LCCO) thin films (x=0.06−0.15% x=0.06-0.15) fabricated by a pulsed laser deposition technique. The in-plane AMR with H∥ab\mathbf{H}\parallel ab shows a twofold symmetry instead of the fourfold behavior found in other electron-doped cuprates such as Pr2−x% _{2-x}Cex_{x}CuO4_{4} and Nd2−x_{2-x}Cex_{x}CuO4_{4}. The twofold AMR disappears above a certain temperature, TDT_{D}. The TD(x)T_{D}(x) is well above Tc(x)T_{c}(x) for x=0.06x=0.06 (∼110\sim 110 K), and decreases with increasing doping, until it is no longer observed above Tc(x)T_{c}(x) at x=0.15x=0.15. This twofold AMR below TD(x)T_{D}(x) is suggested to originate from an antiferromagnetic or spin density wave order.Comment: to be published in Phys. Rev. B, Vol. 80 (2009

    Design and construction of a point-contact spectroscopy rig with lateral scanning capability

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    The design and realization of a cryogenic rig for point-contact spectroscopy measurements in the needle-anvil configuration is presented. Thanks to the use of two piezoelectric nano-positioners, the tip can move along the vertical (zz) and horizontal (xx) direction and thus the rig is suitable to probe different regions of a sample \textit{in situ}. Moreover, it can also form double point-contacts on different facets of a single crystal for achieving, e.g., an interferometer configuration for phase-sensitive measurements. For the latter purpose, the sample holder can also host a Helmholtz coil for applying a small transverse magnetic field to the junction. A semi-rigid coaxial cable can be easily added for studying the behavior of Josephson junctions under microwave irradiation. The rig can be detached from the probe and thus used with different cryostats. The performance of this new probe has been tested in a Quantum Design PPMS system by conducting point-contact Andreev reflection measurements on Nb thin films over large areas as a function of temperature and magnetic field.Comment: 7 pages, 7 figures, published in Rev. Sci. Instru

    Andreev Reflection in Heavy-Fermion Superconductors and Order Parameter Symmetry in CeCoIn_5

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    Differential conductance spectra are obtained from nanoscale junctions on the heavy-fermion superconductor CeCoIn5_5 along three major crystallographic orientations. Consistency and reproducibility of characteristic features among the junctions ensure their spectroscopic nature. All junctions show a similar conductance asymmetry and Andreev reflection-like conductance with reduced signal (~ 10%-13%), both commonly observed in heavy-fermion superconductor junctions. Analysis using the extended Blonder-Tinkham-Klapwijk model indicates that our data provide the first spectroscopic evidence for dx2−y2d_{x^2-y^2} symmetry. To quantify our conductance spectra, we propose a model by considering the general phenomenology in heavy fermions, the two-fluid behavior, and an energy-dependent density of states. Our model fits to the experimental data remarkably well and should invigorate further investigations.Comment: 4 pages, 4 figures; Phys. Rev. Lett., published versio
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