Charge fluctuations across the pressure-induced quantum phase transition in EuCu2(Ge1xSix)2

Mahmoud A. Ahmida, Martin K. Forthaus, Christoph Geibel, Zakir Hossain, Giovanni R. Hearne, Jirka Kaštil, Jiri Prchal, Vladimir Sechovský, and Mohsen M. Abd-Elmeguid
Phys. Rev. B 101, 205127 – Published 18 May 2020
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Abstract

Pressurizing strategically selected compositions of the EuCu2(Ge1xSix)2 series affords an opportunity for gaining microscopic insight into the ground-state properties and interplay between magnetism and valence fluctuations across a quantum critical point. This is investigated by way of systematic Eu151 Mössbauer spectroscopy measurements on x=0 and x=0.5 compositions in the series, pressurized up to 7 GPa including variable temperature scans in the range 300–4.2 K. In EuCu2Ge2 the temperature and pressure dependences of the hyperfine interaction parameters indicate that both the magnetic and divalent state, Euν+ where ν=2, are stable up to 6–7 GPa, thus serving as a useful reference. Whereas in the x=0.5 composition which initially involves Eu2+, collapse of the magnetically ordered state is onset at ∼1.3 GPa and there is emergence of a nonmagnetic intermediate valence state coexisting with the magnetically ordered state. This regime of mixed states is a precursor of a quantum phase transition to a nonmagnetic homogeneous intermediate valence state ν2.45, across a quantum critical point at 3.6 GPa, suggesting a first-order phase transition. X-ray-diffraction pressure studies at 300 K up to 6 GPa of the x=0.5 composition indicate there is no change in lattice symmetry from the tetragonal ThCr2Si2-type structure. There are also no obvious discontinuities in pressure dependences of the lattice parameters upon evolving through the quantum critical point at 3.6 GPa. Increasing pressure changes the starting Eu2+ valence monotonically, until the mean valence attains its largest value ν2.45 indicative of enhanced charge fluctuations at the quantum critical point and plateaus thereafter. High-pressure resistance measurements at low temperatures down to 40 mK near the quantum critical point reveal no evidence for superconductivity.

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  • Received 6 March 2020
  • Revised 23 April 2020
  • Accepted 23 April 2020

DOI:https://doi.org/10.1103/PhysRevB.101.205127

©2020 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

Mahmoud A. Ahmida1,*, Martin K. Forthaus1, Christoph Geibel2, Zakir Hossain3, Giovanni R. Hearne4, Jirka Kaštil5, Jiri Prchal6, Vladimir Sechovský6, and Mohsen M. Abd-Elmeguid1,†

  • 1II. Physikalisches Institut, Universität zu Köln, Zülpicher Str. 77, 50937 Köln, Germany
  • 2Max-Planck-Institute for Chemical Physics of Solids, Nöthnitzer Str. 40, 01187 Dresden, Germany
  • 3Department of Physics, Indian Institute of Technology, Kanpur 208016, India
  • 4Department of Physics, University of Johannesburg, PO Box 524, Auckland Park, 2006, Johannesburg, South Africa
  • 5Institute of Physics, Academy of Sciences of the Czech Republic, Na Slovance 1999/2, Prague 8, Czech Republic
  • 6Department of Condensed Matter Physics, Faculty of Mathematics and Physics, Charles University, Ke Karlovu 5, Prague 2, Czech Republic

  • *Present address: Electrical Engineering Department, The Higher Institute of Sciences and Technology, Ajdabiya, Libya.
  • Corresponding author: meguid@ph2.uni-koeln.de

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Issue

Vol. 101, Iss. 20 — 15 May 2020

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