Jul 7 – 11, 2025
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Electronic and Magnetic Properties of EuZn$_2$P$_2$ Under Pressure

7O-02
Jul 9, 2025, 9:45 AM
15m
ORAL Topic 7 - Rare-earth and 5f-systems Section S7

Speaker

Jiří Kaštil (FZU - Institute of Physics of the Czech Academy of Sciences)

Description

EuZn$_{2}$P$_{2}$ is a narrow-gap semiconductor (0.11 eV) belonging to the Zintl phase family, characterized by mixed ionic and covalent bonding. Although long-range antiferromagnetic order is established only below $23$ K, strong short-range magnetic correlations significantly reduce electrical resistivity well above the ordering temperature, leading to a giant magnetoresistance effect.

The nature of magnetic interactions in EuZn$_{2}$P$_{2}$ remains under debate. We investigated the pressure dependence of the magnetic ordering temperature using DC magnetization measurements in a miniature diamond anvil cell made from nonmagnetic CuBe alloy. Our magnetization measurements reveal a linear increase in magnetization up to $\sim 4$ GPa, followed by a steeper linear rise up to 10 GPa, the limit of our experiment. Notably, no distinct anomaly in electrical resistivity accompanies magnetic ordering. The Néel temperature ($T_N$) at elevated pressures does not correlate with specific features in $R(T)$. Interestingly, the maximum in $R(T)$, although magnetism-related, appears at temperatures higher than the actual T$_N$ at corresponding pressures. We attribute this deviation from an exponentially increasing resistivity trend to magnetic fluctuations that induce the formation of magnetic polarons.

Hydrostatic pressure strongly enhances both the magnetic ordering temperature and the characteristic temperature of short-range magnetic correlations. As pressure increases, the band gap of EuZn$_{2}$P$_{2}$ gradually closes, and the material exhibits metallic-like behavior above $18$ GPa. The giant magnetoresistance effect remains significant even in this high-pressure metallic state and persists up to room temperature. The results suggest that above $18$ GPa, EuZn$_{2}$P$_{2}$ transitions into a ferromagnetically ordered metallic state.

Acknowledgements

The work has been supported by the Czech Science Foundation under the Grants No. 25-16339S. Experiments were performed in MGML (mgml.eu), which is supported within the program of the Czech Research Infrastructures (Project No. LM2023065).

Primary author

Dr U. Dutta (FZU - Institute of Physics of the Czech Academy of Sciences, Prague 8, Czech Republic)

Co-authors

Dr L. Havela (Charles University, Faculty of Mathematics and Physics, Department of Condensed Matter Physics, Ke Karlovu 3, 121 16 Prague 2, Czech Republic) Dr V. Buturlim (Charles University, Faculty of Mathematics and Physics, Department of Condensed Matter Physics, Ke Karlovu 3, 121 16 Prague 2, Czech Republic) Dr J. Prchal (Charles University, Faculty of Mathematics and Physics, Department of Condensed Matter Physics, Ke Karlovu 3, 121 16 Prague 2, Czech Republic) Dr M. Diviš (Charles University, Faculty of Mathematics and Physics, Department of Condensed Matter Physics, Ke Karlovu 3, 121 16 Prague 2, Czech Republic) Dr P. Král (FZU - Institute of Physics of the Czech Academy of Sciences, Prague 8, Czech Republic) Dr I. Turek (Charles University, Faculty of Mathematics and Physics, Department of Condensed Matter Physics, Ke Karlovu 3, 121 16 Prague 2, Czech Republic) Dr I. Halevy (Ben Gurion university, Be’er Sheva, Israel) Jiří Kaštil (FZU - Institute of Physics of the Czech Academy of Sciences) Dr M. Míšek (FZU - Institute of Physics of the Czech Academy of Sciences, Prague 8, Czech Republic) Dr D. Rybicki (GH University of Krakow, Faculty of Physics and Applied Computer Science, Kraków, Poland)

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