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Effect of different in-chain impurities on the magnetic properties of the spin chain compound SrCuO2 probed by NMR

Yannic Utz, Franziska Hammerath, Roberto Kraus, Tobias Ritschel, Jochen Geck, Liviu Hozoi, Jeroen van den Brink, Ashwin Mohan, Christian Hess, Koushik Karmakar, Surjeet Singh, Dalila Bounoua, Romuald Saint-Martin, Loreynne Pinsard-Gaudart, Alexandre Revcolevschi, Bernd Büchner, and Hans-Joachim Grafe
Phys. Rev. B 96, 115135 – Published 19 September 2017

Abstract

The S=1/2 Heisenberg spin chain compound SrCuO2 doped with different amounts of nickel (Ni), palladium (Pd), zinc (Zn), and cobalt (Co) has been studied by means of Cu nuclear magnetic resonance (NMR). Replacing only a few of the S=1/2 Cu ions with Ni, Pd, Zn, or Co has a major impact on the magnetic properties of the spin chain system. In the case of Ni, Pd, and Zn an unusual line broadening in the low temperature NMR spectra reveals the existence of an impurity-induced local alternating magnetization (LAM), while strongly decaying spin-lattice relaxation rates T11 towards low temperatures indicate the opening of spin gaps. A distribution of gap magnitudes is implied by a stretched spin-lattice relaxation and a variation of T11 within the broad resonance lines. These observations depend strongly on the impurity concentration and therefore can be understood using the model of finite segments of the spin 1/2 antiferromagnetic Heisenberg chain, i.e., pure chain segmentation due to S=0 impurities. This is surprising for Ni as it was previously assumed to be a magnetic impurity with S=1 which is screened by the neighboring copper spins. In order to confirm the S=0 state of the Ni, we performed x-ray absorption spectroscopy (XAS) and compared the measurements to simulated XAS spectra based on multiplet ligand-field theory. Furthermore, Zn doping leads to much smaller effects on both the NMR spectra and the spin-lattice relaxation rates, indicating that Zn avoids occupying Cu sites. For magnetic Co impurities, T11 does not obey the gaplike decrease, and the low-temperature spectra get very broad. This could be related to an increase of the Néel temperature and is most likely an effect of the impurity spin S0.

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  • Received 23 May 2017
  • Revised 8 September 2017

DOI:https://doi.org/10.1103/PhysRevB.96.115135

©2017 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

Yannic Utz1, Franziska Hammerath1,2, Roberto Kraus1, Tobias Ritschel2, Jochen Geck2, Liviu Hozoi1, Jeroen van den Brink1,3, Ashwin Mohan1,*, Christian Hess1, Koushik Karmakar4,†, Surjeet Singh4, Dalila Bounoua5, Romuald Saint-Martin5, Loreynne Pinsard-Gaudart5, Alexandre Revcolevschi5, Bernd Büchner1,2, and Hans-Joachim Grafe1

  • 1IFW Dresden, Helmholtzstraße 20, 01069 Dresden, Germany
  • 2Institut für Festkörper- und Materialphysik, Technische Universität Dresden, 01062 Dresden, Germany
  • 3Institut für Theoretische Physik, Technische Universität Dresden, 01062 Dresden, Germany
  • 4Indian Institute of Science Education and Research, Pune, Maharashtra-411008, India
  • 5SP2M-ICMMO, UMR-CNRS 8182, Universit Paris-Sud, Universit Paris-Saclay, 91405 Orsay, France

  • *Present address: Institute of Chemical Technology, Mumbai-400019, India.
  • Present address: IFW Dresden, Helmholtzstraße 20, 01069 Dresden, Germany.

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Issue

Vol. 96, Iss. 11 — 15 September 2017

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Images

  • Figure 1
    Figure 1

    Complete Cu NMR spectra of SrCu0.99Ni0.01O2 at 300 K and 50 K as examples. They have been obtained with a fixed frequency of 80 MHz by varying the magnetic field H while keeping it parallel to the crystallographic b axis (perpendicular to the chains). The normal set of Cu NMR lines and the additional set due to a local lattice distortion around the nickel impurities are marked.

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  • Figure 2
    Figure 2

    Cu63 high-field satellite of SrCuO2, SrCu1xZnxO2, SrCu1xNixO2, and SrCu0.99Co0.01O2 measured with a fixed frequency of 80MHz by varying the magnetic field H||b. The black dashed lines (more precise: their intersections with the base lines of the spectra) indicate the 1/(T) behavior, which is expected for the shoulder feature from the model of semi-infinite chains with (T)ΔH/2H0=0.0326. The plots of the pure, Zn-doped, and Ni-doped samples are arranged such that they show increasing impurity effects from the left to the right (see text). All spectra are normalized to the maximal intensity.

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  • Figure 3
    Figure 3

    Spectra simulated based on the model of finite-sized chain segments (see text). The spectra are each normalized to their maximum. The last panel shows the contribution of chain segments with even and odd number of sites separately.

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  • Figure 4
    Figure 4

    XAS at the Ni L2/3 edge for a sample with 1% Ni doping compared to multiplet calculations for a high spin [left panel: (a), (c), and (e)] and low spin [right panel: (b), (d), and (f)] ground state. (a) and (b) correspond to a polarization of the incident light parallel to the CuO2 plane, whereas (c) and (d) show the XAS for incident light polarization perpendicular to the CuO2 plane. In (e) and (f) the linear dichroism is shown. Blue thick lines represent the experimental data (equal in left and right panel) and red thin lines correspond to the result from multiplet ligand-field theory.

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  • Figure 5
    Figure 5

    Spin-lattice relaxation rates and stretching exponents λ of SrCu1xNixO2 for varying x measured on the center of the Cu63 high-field satellite and T11 of pure SrCuO2 measured on the central transition for comparison. While all doped samples were measured with the magnetic field μ0H7T parallel to the crystallographic c axis (parallel to the chains), the values of the pure compound were obtained with the magnetic field parallel to the a axis (perpendicular to the chains). T11 values measured with a||H are scaled. The black arrows indicate the crossover temperatures T*.

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  • Figure 6
    Figure 6

    Frequency-dependent spin-lattice relaxation measurement on the Cu63 high-field satellite of SrCu0.99Ni0.01O2 (a) and of SrCu0.99Zn0.02O2 (b) at different temperatures. T11 (filled black squares), stretching exponents λ (open cyan circles), and spectrum (dark gold line) were measured with the b axis parallel to the field μ0H=6.9981T (a) and μ0H=7.0488T (b). The spectral intensity is normalized to the maximum of the high-field satellite and its scale is not shown in the graph.

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  • Figure 7
    Figure 7

    NMR spectra of SrCu0.99Pd0.01O2 at different temperatures measured with a fixed frequency of 80MHz by varying the magnetic field H||b. The spectra of SrCu0.99Ni0.01O2 are plotted as black lines for comparison.

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  • Figure 8
    Figure 8

    T11 and stretching exponents λ of SrCu0.99Pd0.01O2 and SrCu0.99Co0.01O2 and of SrCu0.99Ni0.01O2 and pure SrCuO2 for comparison, each measured on the center of the Cu63 high-field satellite. All samples were measured with the magnetic field μ0H7T parallel to the crystallographic b axis, except of the pure sample which was measured with the magnetic field parallel to the a axis. Both directions are perpendicular to the chains.

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  • Figure 9
    Figure 9

    T11 and stretching exponents λ of SrCu1xZnxO2 for varying x and of SrCu1xNixO2 for comparison, each measured on the center of the Cu63 high-field satellite. All samples were measured with the magnetic field μ0H7T parallel to the crystallographic b axis. The black arrows indicate the crossover temperatures T*.

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