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Magnetic structure in square cupola compound Ba(TiO)Cu$_4$(PO$_4$)$_4$: a $^{31}$P NMR Study

Strongly Correlated Electrons 2020-02-19 v1 Materials Science Chemical Physics

Abstract

The magnetic structure of the antiferromagnetic square cupola compound Ba(TiO)Cu4_4(PO4_4)4_4 with the tetragonal structure is studied with 31P nuclear magnetic resonance techniques. The magnetic hyperfine shift K shows a clear splitting at the N\'eel temperature TN_N = 9.5 K, where the resonance splits into two lines when an external magnetic field is oriented along the c axis and into four lines when the field is along the a axis. In the paramagnetic region K(T) follows temperature dependence of the magnetic susceptibility χ(T)\chi(T). From K vs χ\chi plot we determined nearly isotropic hyperfine field values Ha_hf = 765 mT/μB\mu_B and Hc_hf = 740 mT/μB\mu_B for the magnetic field oriented along a and c, respectively. From the rotation of the single crystal in the external magnetic field we determined eight different orientations of K-tensor in the paramagnetic region. In the 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 the single crystal shows eight different orientations of the local field Bint = 35.6 mT. The orientations correspond to the calculation of dipolar fields at phosphorus assuming magnetic quadrupolar configuration of magnetic moments Γ3(1)\varGamma_3(1) described previously [Nat. Commun. 7, 13039 (2016); Phys. Rev. B 96, 214436 (2017)].

Keywords

Cite

@article{arxiv.1911.07684,
  title  = {Magnetic structure in square cupola compound Ba(TiO)Cu$_4$(PO$_4$)$_4$: a $^{31}$P NMR Study},
  author = {Riho Rästa and Ivo Heinmaa and Kenta Kimura and Tsuyoshi Kimura and Raivo Stern},
  journal= {arXiv preprint arXiv:1911.07684},
  year   = {2020}
}

Comments

9 pages, 12 figures