# Absence of long range order in the frustrated magnet SrDy$_2$O$_4$ due   to trapped defects from a dimensionality crossover

**Authors:** N. Gauthier, A. Fennell, B. Pr\'evost, A.-C. Uldry, B. Delley, R., Sibille, A. D\'esilets-Benoit, H.A. Dabkowska, G. Nilsen, L.-P. Regnault,, J.S. White, C. Niedermayer, V. Pomjakushin, A.D. Bianchi, M. Kenzelmann

arXiv: 1702.02329 · 2017-04-20

## TL;DR

This study investigates why SrDy$_2$O$_4$ remains disordered at very low temperatures, revealing that trapped defects and dimensional crossover prevent long-range magnetic order despite strong 1D correlations.

## Contribution

It demonstrates that trapped domain walls due to dimensional crossover explain the absence of long-range order in SrDy$_2$O$_4$, combining neutron scattering and susceptibility data.

## Key findings

- Strong 1D magnetic correlations along chains
- 3D correlations emerge below 0.7 K
- Absence of long-range order due to trapped domain walls

## Abstract

Magnetic frustration and low dimensionality can prevent long range magnetic order and lead to exotic correlated ground states. SrDy$_2$O$_4$ consists of magnetic Dy$^{3+}$ ions forming magnetically frustrated zig-zag chains along the c-axis and shows no long range order to temperatures as low as $T=60$ mK. We carried out neutron scattering and AC magnetic susceptibility measurements using powder and single crystals of SrDy$_2$O$_4$. Diffuse neutron scattering indicates strong one-dimensional (1D) magnetic correlations along the chain direction that can be qualitatively accounted for by the axial next-nearest neighbour Ising (ANNNI) model with nearest-neighbor and next-nearest-neighbor exchange $J_1=0.3$ meV and $J_2=0.2$ meV, respectively. Three-dimensional (3D) correlations become important below $T^*\approx0.7$ K. At $T=60$ mK, the short range correlations are characterized by a putative propagation vector $\textbf{k}_{1/2}=(0,\frac{1}{2},\frac{1}{2})$. We argue that the absence of long range order arises from the presence of slowly decaying 1D domain walls that are trapped due to 3D correlations. This stabilizes a low-temperature phase without long range magnetic order, but with well-ordered chain segments separated by slowly-moving domain walls.

## Full text

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## Figures

16 figures with captions in the complete paper: https://tomesphere.com/paper/1702.02329/full.md

## References

43 references — full list in the complete paper: https://tomesphere.com/paper/1702.02329/full.md

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Source: https://tomesphere.com/paper/1702.02329