English

Frustration of square cupola in Sr(TiO)Cu$_{4}$(PO$_{4}$)$_{4}$

Materials Science 2018-07-04 v1

Abstract

The structural and magnetic properties of the square-cupola antiferromagnet Sr(TiO)Cu4_{4}(PO4_{4})4_{4} are investigated via x-ray diffraction, magnetization, heat capacity, and 31^{31}P nuclear magnetic resonance experiments on polycrystalline samples, as well as density-functional band-structure calculations. The temperature-dependent unit cell volume could be described well using the Debye approximation with the Debye temperature of θD\theta_{\rm D} \simeq 550~K. Magnetic response reveals a pronounced two-dimensionality with a magnetic long-range-order below TN6.2T_{\rm N} \simeq 6.2~K. High-field magnetization exhibits a kink at 1/31/3 of the saturation magnetization. Asymmetric 31^{31}P NMR spectra clearly suggest strong in-plane anisotropy in the magnetic susceptibility, as anticipated from the crystal structure. From the 31^{31}P NMR shift vs bulk susceptibility plot, the isotropic and axial parts of the hyperfine coupling between 31^{31}P nuclei and the Cu2+^{2+} spins are calculated to be Ahfiso6539A_{\rm hf}^{\rm iso} \simeq 6539 and Ahfax952A_{\rm hf}^{\rm ax} \simeq 952~Oe/μB\mu_{\rm B}, respectively. The low-temperature and low-field 31^{31}P NMR spectra indicate a commensurate antiferromagnetic ordering. Frustrated nature of the compound is inferred from the temperature-dependent 31^{31}P NMR spin-lattice relaxation rate and confirmed by our microscopic analysis that reveals strong frustration of the square cupola by next-nearest-neighbor exchange couplings.

Keywords

Cite

@article{arxiv.1805.07497,
  title  = {Frustration of square cupola in Sr(TiO)Cu$_{4}$(PO$_{4}$)$_{4}$},
  author = {S. S. Islam and K. M. Ranjith and M. Baenitz and Y. Skourski and A. A. Tsirlin and R. Nath},
  journal= {arXiv preprint arXiv:1805.07497},
  year   = {2018}
}

Comments

11 pages, 13 figures, 1 table, Phys. Rev. B (Accepted, 2018)