# High-magnetic field phase diagram and failure of magnetic Gr\"uneisen   scaling in LiFePO$_4$

**Authors:** J. Werner, S. Sauerland, C. Koo, C. Neef, A. Pollithy, Y. Skourski, R., Klingeler

arXiv: 1903.05169 · 2019-07-03

## TL;DR

This study maps the magnetic phase diagram of LiFePO4 up to 58 T, reveals strong magneto-elastic coupling, and shows failure of Grüneisen scaling below 40 K, indicating complex competing degrees of freedom.

## Contribution

It provides the first detailed high-field phase diagram of LiFePO4 and analyzes magneto-elastic effects and magnetic excitations with new quantitative parameters.

## Key findings

- Magnetic phase diagram established up to 58 T.
- Failure of Grüneisen scaling below 40 K.
- Identification of spin-reorientation at 32 T.

## Abstract

We report the magnetic phase diagram of single-crystalline LiFePO$_4$ in magnetic fields up to 58~T and present a detailed study of magneto-elastic coupling by means of high-resolution capacitance dilatometry. Large anomalies at \tn\ in the thermal expansion coefficient $\alpha$ imply pronounced magneto-elastic coupling. Quantitative analysis yields the magnetic Gr\"uneisen parameter $\gamma_{\rm mag}=6.7(5)\cdot 10^{-7}$~mol/J. The positive hydrostatic pressure dependence $dT_{\rm N}/dp = 1.46(11)$~K/GPa is dominated by uniaxial effects along the $a$-axis. Failure of Gr\"uneisen scaling below $\approx 40$~K, i.e., below the peak temperature in the magneto-electric coupling coefficient [\onlinecite{toft2015anomalous}], implies several competing degrees of freedom and indicates relevance of recently observed hybrid excitations~[\onlinecite{yiu2017hybrid}]. A broad and strongly magnetic-field-dependent anomaly in $\alpha$ in this temperature regime highlight the relevance of structure changes. Upon application of magnetic fields $B||b$-axis, a pronounced jump in the magnetisation implies spin-reorientation at $B_{\rm SF} = 32$~T as well as a precursing phase at 29~T and $T=1.5$~K. In a two-sublattice mean-field model, the saturation field $B_{\rm sat,b} = 64(2)$~T enables the determination of the effective antiferromagnetic exchange interaction $J_{\rm af} = 2.68(5)$~meV as well as the anisotropies $D_{\rm b} = -0.53(4)$~meV and $D_{\rm c} = 0.44(8)$~meV.

## Full text

_Full body text omitted from this summary view._ Fetch the complete paper as Markdown: https://tomesphere.com/paper/1903.05169/full.md

## Figures

7 figures with captions in the complete paper: https://tomesphere.com/paper/1903.05169/full.md

## References

30 references — full list in the complete paper: https://tomesphere.com/paper/1903.05169/full.md

---
Source: https://tomesphere.com/paper/1903.05169