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Colossal magnetoresistance in <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:msub><mml:mi>EuZn</mml:mi><mml:mn>2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">P</mml:mi><mml:mn>2</mml:mn></mml:msub></mml:mrow></mml:math> and its electronic and magnetic structure

Sarah Krebber, Marvin Kopp, Charu Garg, K. Kummer, J. Sichelschmidt, Susanne Schulz, G. Poelchen, Max Mende, A.V. Virovets, Konstantin Warawa, Mark D. Thomson, А. В. Тарасов, Dmitry Yu. Usachov, D. V. Vyalikh, Hartmut G. Roskos, Jens Müller, C. Krellner, Kristin Kliemt

2023Physical review. B./Physical review. B27 citationsDOI

Abstract

We investigate single crystals of the trigonal antiferromagnet ${\mathrm{EuZn}}_{2}{\mathrm{P}}_{2}$ ($P\overline{3}m1$) by means of electrical transport, magnetization measurements, x-ray magnetic scattering, optical reflectivity, angle-resolved photoemission spectroscopy (ARPES), and ab initio band structure calculations ($\mathrm{DFT}+U$). We find that the electrical resistivity of ${\mathrm{EuZn}}_{2}{\mathrm{P}}_{2}$ increases strongly upon cooling and can be suppressed in magnetic fields by several orders of magnitude (colossal magnetoresistance effect). Resonant magnetic scattering reveals a magnetic ordering vector of $q=(0\phantom{\rule{0.16em}{0ex}}0\phantom{\rule{0.16em}{0ex}}\frac{1}{2})$, corresponding to an $A$-type antiferromagnetic order, below ${T}_{\mathrm{N}}=23.7\phantom{\rule{0.28em}{0ex}}\mathrm{K}$. We find that the moments are canted out of the $a\text{\ensuremath{-}}a$ plane by an angle of about ${40}^{\ensuremath{\circ}}\ifmmode\pm\else\textpm\fi{}{10}^{\ensuremath{\circ}}$ and aligned along the [100] direction in the $a\text{\ensuremath{-}}a$ plane. We observe nearly isotropic magnetization behavior for low fields and low temperatures which is consistent with the magnetic scattering results. The magnetization measurements show a deviation from the Curie-Weiss behavior below $\ensuremath{\approx}150\phantom{\rule{0.28em}{0ex}}\mathrm{K}$, the temperature below which also the field dependence of the material's resistivity starts to increase. An analysis of the infrared reflectivity spectrum at $T=295\phantom{\rule{0.28em}{0ex}}\mathrm{K}$ allows us to resolve the main phonon bands and intraband and interband transitions, and estimate indirect and direct band gaps of ${E}_{i}^{\mathrm{opt}}=0.09$ and ${E}_{d}^{\mathrm{opt}}=0.33\phantom{\rule{0.28em}{0ex}}\mathrm{eV}$, respectively, which are in good agreement with the theoretically predicted ones. The experimental band structure obtained by ARPES is nearly $T$ independent above and below ${T}_{\mathrm{N}}$. The comparison of the theoretical and experimental data shows a weak intermixing of the Eu $4f$ states close to the $\mathrm{\ensuremath{\Gamma}}$ point with the bands formed by the phosphorous $3p$ orbitals leading to an induction of a small magnetic moment at the P sites.

Topics & Concepts

Condensed matter physicsMagnetizationAntiferromagnetismPhysicsScatteringAngle-resolved photoemission spectroscopyMagnetoresistanceMagnetic fieldElectronic structureOpticsQuantum mechanicsRare-earth and actinide compoundsPhysics of Superconductivity and MagnetismIron-based superconductors research
Colossal magnetoresistance in <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:msub><mml:mi>EuZn</mml:mi><mml:mn>2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">P</mml:mi><mml:mn>2</mml:mn></mml:msub></mml:mrow></mml:math> and its electronic and magnetic structure | Litcius