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Published on: June 28, 2018
EuFe2(As(1-x)P(x))2: reentrant spin glass and superconductivity.
S Zapf1, H S Jeevan2, T Ivek1
11. Physikalisches Institut, Universität Stuttgart, Pfaffenwaldring 57, 70550 Stuttgart, Germany.
This study reveals that superconductivity coexists with a reentrant spin glass state in EuFe(2)(As(1-x)P(x))(2) materials, particularly around x≈0.2. This finding revises the understanding of magnetic transitions and their interplay with superconductivity.
Area of Science:
- Condensed Matter Physics
- Materials Science
- Magnetism and Superconductivity
Background:
- Investigating the interplay between magnetism and superconductivity is crucial for understanding complex electronic phases.
- EuFe(2)(As(1-x)P(x))(2) is a promising material system for exploring such phenomena due to the presence of Eu(2+) magnetism.
Purpose of the Study:
- To systematically investigate the magnetic, transport, and thermodynamic properties of EuFe(2)(As(1-x)P(x))(2) single crystals.
- To explore the complex interplay between Eu(2+) magnetism and superconductivity across the entire substitution range (0≤x≤1).
Main Methods:
- Synthesis of single crystals of EuFe(2)(As(1-x)P(x))(2) for 0≤x≤1.
- Systematic measurements of magnetic, transport, and thermodynamic properties.
- Analysis of magnetic transitions and their coexistence with superconducting properties.
Main Results:
- Two distinct magnetic transitions were observed below 30 K for all P-substituted crystals, necessitating a revised phase diagram.
- A canted A-type antiferromagnetic order of Eu(2+) at ~20 K and a spin glass transition at lower temperatures were identified.
- Remarkably, a reentrant spin glass state was found to coexist with superconductivity around x≈0.2.
Conclusions:
- The study revises the phase diagram of EuFe(2)(As(1-x)P(x))(2) by revealing new magnetic transitions.
- The coexistence of superconductivity with a reentrant spin glass state in this system presents a novel finding.
- These results offer critical insights into the complex interplay between magnetism and superconductivity in correlated electron systems.
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