Hole-Doping Effect on the Spin State and Microscopic Magnetic Properties of La1-xSrxCoO3(0≦x≦0.5)--59Co and 139La NMR Measurements

  • Itoh Masayuki
    Department of Physics, Faculty of Science, Chiba University, Yayoi–cho, Inage–ku, Chiba 263
  • Natori Ikuomi
    Department of Physics, Faculty of Science, Chiba University, Yayoi–cho, Inage–ku, Chiba 263

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  • Hole-Doping Effect on the Spin State and Microscopic Magnetic Properties of La1-xSrxCoO3 (0.LEQ.x.LEQ.0.5): 59Co and 139La NMR Measurements.
  • Hole Doping Effect on the Spin State an
  • Hole-Doping Effect on the Spin State and Microscopic Magnetic Properties of<b><i>L</i><i>a</i><sub>1-<i>x</i></sub><i>S</i><i>r</i><sub><i>x</i></sub><i>C</i><i>o</i><i>O</i><sub>3</sub></b>(0≤<i><i>x</i></i>≤0.5):<b><sup>59</sup><i>C</i><i>o</i></b>and<b><sup>139</sup><i>L</i><i>a</i></b>NMR Measurements

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59Co and 139La NMR measurements have been made to reveal microscopically the hole-doping effect on the spin state and magnetic properties of La1-xSrxCoO3 (0{\le}x{\le}0.5). The signal from the Co atoms with no Sr nearest neighbors was observed in the spin-glass region below xc--0.18. From the analysis of the temperature dependence of the Knight shift, the ground state of such Co atoms was found to be the trivalent low-spin state 1A1g. Above xc, we observed at 4.2, K the 59Co and 139La signals which come from the cluster-glass region with a finite ferromagnetic correlation. Thus, it was microscopically confirmed that the boundary between the two regions is located at xc--0.18.

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