Competing 4f-electron dynamics in Ce(Ru1-xFex) 2Al10 (0≤x≤1.0): Magnetic ordering emerging from the Kondo semiconducting state

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dc.contributor.author Adroja, D. T.
dc.contributor.author Hillier, A. D.
dc.contributor.author Muro, Y.
dc.contributor.author Kajino, J.
dc.contributor.author Takabatake, T.
dc.contributor.author Peratheepan, P.
dc.contributor.author Strydom, A. M.
dc.contributor.author Deen, P. P.
dc.contributor.author Demmel, F.
dc.contributor.author Stewart, J. R.
dc.contributor.author Taylor, J. W.
dc.contributor.author Smith, R. I.
dc.contributor.author Ramos, S.
dc.contributor.author Adams, M.A.
dc.date.accessioned 2019-08-11T04:31:40Z
dc.date.available 2019-08-11T04:31:40Z
dc.date.issued 2013
dc.identifier.uri http://www.digital.lib.esn.ac.lk/handle/123456789/3967
dc.description.abstract We have carried out muon spin relaxation (muSR), 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 muSR spectra clearly reveal coherent two-frequency oscillations at low temperature in x=0, 0.3 and 0.5 samples, which confirms the long-range magnetic ordering of the Ce-moment with TN=27, 26 and 21 K respectively. On the other hand the muSR 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 Q-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 hybridization gap opening only a small part of the Fermi surface, gapped spin waves, or a spin-dimer gap. en_US
dc.language.iso en en_US
dc.publisher Physical Review en_US
dc.subject Magnetic excitations en_US
dc.subject Spin gap en_US
dc.subject Kondo semiconductor en_US
dc.subject Antiferromagnetic phase transition en_US
dc.subject Ce(Ru1-xFex)2Al10 en_US
dc.subject Muon spin relaxation en_US
dc.subject Reduced moment magnetic ordering en_US
dc.subject Inelastic neutron scattering en_US
dc.title Competing 4f-electron dynamics in Ce(Ru1-xFex) 2Al10 (0≤x≤1.0): Magnetic ordering emerging from the Kondo semiconducting state en_US
dc.type Article en_US
dc.identifier.sslno 05 en_US


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