journal article·2021-02-01

High magnetic anisotropy and magnon excitations in single crystals of the double spin chain compound PbMn2Ni6Te3O18

I. Panneer Muthuselvam, K. Saranya, Florian Büscher, Dirk Wulferding, Peter Lemmens, Wei-tin Chen, R. Sankar

Physical Review B· Volume 103· Issue 6
Publisher page

Abstract

We have successfully grown single crystals of $\mathrm{Pb}{\mathrm{Mn}}2{\mathrm{Ni}}6{\mathrm{Te}}3{\mathrm{O}}18$ and present a comprehensive study of their magnetic, thermodynamic, and Raman spectroscopic properties. $\mathrm{Pb}{\mathrm{Mn}}2{\mathrm{Ni}}6{\mathrm{Te}}3{\mathrm{O}}18$ consists of a planar network of pairwise rotated $\mathrm{Ni}{\mathrm{O}}6$ dimers coupled by corners. Similarities to ${\mathrm{Ni}}3\mathrm{Te}{\mathrm{O}}6$ exist, which forms honeycomb layers. The magnetic susceptibility \ensuremath{\chi} and heat capacity ${C}p$ data reveal an antiferromagnetic phase transition around 84 K, which is evidently hysteretic on warming and cooling between 94 and 40 K with a loop width of about 1.83\ifmmode\pm\else\textpm\fi{} 0.41 K; thus the transition appears to be of first order. \ensuremath{\chi} is anisotropic, with larger values for in-plane fields over the entire measured temperature range. Raman spectroscopy has been employed to investigate the lattice and magnetic excitations of the $\mathrm{Pb}{\mathrm{Mn}}2{\mathrm{Ni}}6{\mathrm{Te}}3{\mathrm{O}}18$ from 5 to 300 K. Besides an anharmonic phonon behavior, i.e., a decay into acoustic phonons, we find a coupling to the spin system at ${T}N=84\phantom{\rule{0.16em}{0ex}}\mathrm{K}$, as well as weak anomalies at ${T}*\ensuremath{\approx}200\phantom{\rule{0.16em}{0ex}}\mathrm{K}$. This second characteristic temperature gives evidence for an instability of the coupled spin/lattice system, as here the phonon linewidths and intensities evidence similar behavior as at ${T}N=84\phantom{\rule{0.16em}{0ex}}\mathrm{K}$. Furthermore, magnetic Raman scattering at $240\phantom{\rule{0.16em}{0ex}}\mathrm{c}{\mathrm{m}}^{\ensuremath{-}1}$ is used to estimate an exchange coupling of $J=--86\phantom{\rule{0.16em}{0ex}}\mathrm{K}$ in general agreement with the Curie-Weiss temperature.
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Research context

OpenAlex topics: Advanced Condensed Matter Physics · Multiferroics and related materials · Magnetic and transport properties of perovskites and related materials

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References (15)

Show source-provided references
1. 10.1016/0375-9601(83)90631-X10.1016/0375-9601(83)90631-X ↗
2. 10.1103/PhysRevLett.50.115310.1103/PhysRevLett.50.1153 ↗
3. 10.1103/PhysRevLett.56.37110.1103/PhysRevLett.56.371 ↗
4. 10.1103/PhysRevB.38.54310.1103/PhysRevB.38.543 ↗
5. 10.1103/PhysRevLett.73.185710.1103/PhysRevLett.73.1857 ↗
6. 10.1103/PhysRevB.54.643710.1103/PhysRevB.54.6437 ↗
7. 10.1103/PhysRevB.54.721010.1103/PhysRevB.54.7210 ↗
8. 10.1016/S0025-5408(99)00231-710.1016/S0025-5408(99)00231-7 ↗
9. 10.1021/acs.inorgchem.5b0161910.1021/acs.inorgchem.5b01619 ↗
10. 10.1088/0953-8984/27/45/45600110.1088/0953-8984/27/45/456001 ↗
11. 10.1103/PhysRevB.95.07510510.1103/PhysRevB.95.075105 ↗
12. J. Weidlein · 1981
13. 1986
14. 10.1103/PhysRevB.95.18443510.1103/PhysRevB.95.184435 ↗
15. 10.1103/PhysRevB.84.14410110.1103/PhysRevB.84.144101 ↗