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Competing4f-electron dynamics in Ce(Ru1?xFex)2Al10(0?x?1.0): Magnetic ordering emerging from the Kondo semiconducting state

Adroja, D. T., Hillier, A. D., Muro, Y., Kajino, J., Takabatake, T., Peratheepan, P., Strydom, A. M., Deen, P. P., Demmel, F., Stewart, J. R., and others. (2013) Competing4f-electron dynamics in Ce(Ru1?xFex)2Al10(0?x?1.0): Magnetic ordering emerging from the Kondo semiconducting state. Physical Review B, 87 (22). p. 224415. ISSN 1098-0121. (doi:10.1103/PhysRevB.87.224415) (The full text of this publication is not currently available from this repository. You may be able to access a copy if URLs are provided)

The full text of this publication is not currently available from this repository. You may be able to access a copy if URLs are provided. (Contact us about this Publication)
Official URL
http://doi.org/10.1103/PhysRevB.87.224415

Abstract

We have carried out muon spin relaxation (?SR), neutron diffraction, and inelastic neutron scattering (INS) investigations on polycrystalline samples of Ce(Ru1?xFex)2Al10 (x=0, 0.3, 0.5, 0.8, and 1) to investigate the nature of the ground state (magnetic ordered versus paramagnetic) and the origin of the spin-gap formation as evident from the bulk measurements in the end members. Our zero-field ?SR spectra clearly reveal coherent two-frequency oscillations at low temperature in x=0, 0.3, and 0.5 samples, which confirm the long-range magnetic ordering of the Ce moment with Nèel temperature TN=27, 26, and 21 K, respectively. On the other hand, the ?SR spectra of x=0.8 and x=1 down to 1.4 K and 0.045 K, respectively, exhibit a temperature-independent Kubo-Toyabe term, confirming a paramagnetic ground state. The long-range magnetic ordering in x=0.5 below 21 K has been confirmed through the neutron diffraction study. INS measurements of x=0 clearly reveal the presence of a sharp inelastic excitation near 8 meV between 5 K and 26 K, due to an opening of a gap in the spin excitation spectrum, which transforms into a broad response at and above 30 K. Interestingly, at 4.5 K, the spin-gap excitation broadens in x=0.3 and exhibits two clear peaks at 8.4(3) and 12.0(5) meV in x=0.5. In the x=0.8 sample, which remains paramagnetic down to 1.2 K, there is a clear signature of a spin gap of 10–12 meV at 7 K, with a strong wave-vector–dependent intensity. Evidence of a spin gap of 12.5(5) meV has also been found in x=1. The observation of a spin gap in the paramagnetic samples (x=0.8 and 1) is an interesting finding in this study, and it challenges our understanding of the origin of the semiconducting gap in CeT2Al10 (T = Ru and Os) compounds in terms of a hybridization gap opening only a small part of the Fermi surface, gapped spin waves, or a spin-dimer gap.

Item Type: Article
DOI/Identification number: 10.1103/PhysRevB.87.224415
Uncontrolled keywords: Physics of Quantum Materials
Subjects: Q Science > QC Physics > QC176 Solid state physics
Divisions: Faculties > Sciences > School of Physical Sciences > Functional Materials Group
Depositing User: Silvia Ramos
Date Deposited: 28 Apr 2015 10:25 UTC
Last Modified: 17 Jul 2019 09:57 UTC
Resource URI: https://kar.kent.ac.uk/id/eprint/48083 (The current URI for this page, for reference purposes)
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