Pressure evolution of the electronic structure of non-centrosymmetric EuRhGe₃

Abstract

Among europium compounds, pressure induced valence transitions and/or intermediate valence states are often observed. In such systems, applying pressure of several GPa can drive a Eu valence from divalent to almost trivalent. Non-centrosymmetric EuRhGe3 possesses magnetic Eu2+ ions and exhibits antiferromagnetic ordering at ∼11 K at ambient pressure. Pressure resistant magnetic ordering and stable divalent Eu state have been reported in EuRhGe3. Here, we study the pressure evolution of the Eu valence of EuRhGe3 by high resolution x-ray absorption spectroscopy using the partial fluorescence yield method. Our study reveals a successive increase of the Eu valence with increasing pressure without any valence transition. The obtained mean Eu valence approaches ∼2.4 around 40 GPa at 300 K. The experimental data are also analyzed by a full multiplet configuration interaction calculation based on the single impurity Anderson model. The analysis reveals a decrease of the Eu 4f orbital occupation by applying pressure. Pressure evolution of the electronic structure studied by density functional theory suggests that the Rh ions have little contribution to the pressure evolution of the Eu valence, while it implies an active involvement of the Ge ions.

Magnetic properties of the noncentrosymmetric tetragonal antiferromagnet EuPtSi$_{3}$

“…A candidate for such behavior is EuPtSi 3 , belonging to a class of europium-based compounds crystallizing in the noncentrosymmetric tetragonal space group I4mm [19][20][21][22][23][24][25][26][27][28][29][30][31][32]. In a seminal study, Kumar and colleagues investigated single-crystal platelets grown from a tin solution [33].…”

Cycloidal Magnetic Ordering in Noncentrosymmetric EuIrGe3

“…[20][21][22][23][24] The magnetic properties of EuRhGe 3 and EuIrGe 3 have also been well studied. [25][26][27] In spite of weak magnetic anisotropies of Eu 2+ , these compounds exhibit multiple magnetic phases in the temperature (T ) vs magnetic field (H) space, suggesting a subtle energy balance among various magnetic structures, which is of great interest. EuIrGe 3 , the subject compound of this paper, exhibits successive phase transitions at T N =12.2 K, T ′ N =7.0 K, and T * N =5.0 K. 18,26) The crystal structure and the physical properties of EuIrGe 3 are summarized in Fig.…”