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Magnetic and transport properties in CoSr2Y1xCaxCu2O7 (x=00.4)

X. G. Luo, X. H. Chen, X. Liu, R. T. Wang, Y. M. Xiong, C. H. Wang, G. Y. Wang, and X. G. Qiu
Phys. Rev. B 70, 054520 – Published 31 August 2004

Abstract

Magnetic and transport properties of CoSr2Y1xCaxCu2O7 (x=00.4) system have been investigated. A broad maximum in the M(T) curve, indicative of low-dimensional antiferromagnetic ordering originated from CoO1+δ layers, is observed in the Ca-free sample. With increasing as Ca doping level up to 0.2, the M(T) curve remains almost unchanged, while resistivity is reduced by three orders. A higher Ca doping level leads to a drastic change of magnetic properties. In comparison with the samples with x=0.00.2, the temperature corresponding to the maximum of M(T) is much lower for the sample x=0.3. The sample x=0.4 shows a small kink instead of a broad maximum and a weak ferromagnetic feature. The electrical transport behavior is found to be closely related to magnetic properties for the sample x=0.2, 0.25, 0.3, 0.4. It suggests that CoO1+δ layers are involved in charge transport, in addition to conducting CuO2 planes to interpret the correlation between magnetism and charge transport. X-ray photoelectron spectroscopy studies give additional evidence of the the transfer of the holes into the CoO1+δ charge reservoir.

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  • Received 2 January 2004

DOI:https://doi.org/10.1103/PhysRevB.70.054520

©2004 American Physical Society

Authors & Affiliations

X. G. Luo, X. H. Chen*, X. Liu, R. T. Wang, Y. M. Xiong, C. H. Wang, and G. Y. Wang

  • Structure Research Laboratory and Department of Physics, University of Science and Technology of China, Hefei, Anhui, 230026, People's Republic of China

X. G. Qiu

  • State Key Laboratory of Superconductivity, Institute of Physics, Chinese Academy of Sciences, Beijing 10080, People’s Republic of China

  • *Electronic address: chenxh@ustc.edu.cn

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Vol. 70, Iss. 5 — 1 August 2004

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Images

  • Figure 1
    Figure 1
    XRD patterns for the as-synthesized samples of CoSr2Y1xCaxCu2O7+δ(x=0.00.4).Reuse & Permissions
  • Figure 2
    Figure 2
    Lattice parameters for the as-synthesized samples of CoSr2Y1xCaxCu2O7+δ.Reuse & Permissions
  • Figure 3
    Figure 3
    (a) The temperature dependence of magnetization measured for the annealed CoSr2Y1xCaxCu2O7+δ samples in field-cooled process at the field of 100Oe. Inset: ZFC (dashed line) and FC (solid line) data at the field of 100Oe plotted against the temperature for the samples x=0.25 and 0.4. (b) The temperature dependence of inverse magnetization for the sample x=0.00.4.Reuse & Permissions
  • Figure 4
    Figure 4
    The resistivity as a function of temperature for the annealed CoSr2Y1xCaxCu2O7+δ samples.Reuse & Permissions
  • Figure 5
    Figure 5
    The resistivity and its derivative as a function of temperature for the samples with x=0.2, 0.25, 0.3, 0.4.Reuse & Permissions
  • Figure 6
    Figure 6
    The temperature dependence of the resistivity curvature (d2ρd2T) and magnetization for the samples with x=0.2, 0.25, 0.3, 0.4.Reuse & Permissions
  • Figure 7
    Figure 7
    The plot of magnetoresistance (MR=[ρ(T,H)ρ(T,0)]ρ(T,0)×100%) vs magnetic field (μ0H) for the samples with x=0.3, 0.4. Insets: the same data are shown in Kohler’s plot.Reuse & Permissions
  • Figure 8
    Figure 8
    The Co2p XPS spectra for the sample x=0.1 and 0.4.Reuse & Permissions
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