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Magnetic structure in square cupola compound Ba(TiO)Cu<sub>4</sub>(PO<sub>4</sub>)<sub>4</sub>: <sup>31</sup>P NMR Study

ORAL

Abstract

The magnetic structure of the antiferromagnetic square cupola compound Ba(TiO)Cu4(PO4)4 single crystal is studied with 31P nuclear magnetic resonance techniques. The magnetic hyperfine shift K shows a clear splitting at the Neel temperature TN = 9.5 K, where the resonance splits into 2 lines when the external field is oriented along c-axis and into 4 lines when the field is along a-axis. In paramagnetic region K(T) follows temperature dependence of the magnetic susceptibility χ(T). From K vs χ plot we determined hyperfine field values Hahf = 765 mT/μB and Hchf = 740 mT/μB for magnetic field oriented along a- and c-axis, respectively. From the rotation of the single crystal in external magnetic field we determined 8 different orientations of K-tensor in paramagnetic region. In antiferromagnetic state at T = 6 K we found that the local field at phosphorus is mainly due to dipolar field of coppers. Here the rotation of single crystal shows 8 different orientations of the local field Bint = 38 ± 2 mT. Experimental orientation of Bint corresponds to the calculation of dipolar fields at phosphorus assuming magnetic quadrupolar configuration of magnetic moments Γ3(1).

Presenters

  • Raivo Stern

    NICBP, Tallinn, Chemical Physics, National Institute of Chemical Physics and Biophysics, Tallinn, Estonia

Authors

  • Raivo Stern

    NICBP, Tallinn, Chemical Physics, National Institute of Chemical Physics and Biophysics, Tallinn, Estonia

  • Ivo Heinmaa

    Chemical Physics, National Institute of Chemical Physics and Biophysics, Tallinn, Estonia

  • Riho Rästa

    Chemical Physics, National Institute of Chemical Physics and Biophysics, Tallinn, Estonia

  • Kenta Kimura

    Advanced Materials Science, University of Tokyo, Kashiwa, Japan

  • Tsuyoshi Kimura

    Advanced Materials Science, University of Tokyo, Kashiwa, Japan