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2016
DOI: 10.1016/j.jmmm.2015.07.043
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Spin-excitons in heavy-fermion semimetals

Abstract: Spin-excitons are sharp and dispersive magnetic fluctuations in paramagnetic semiconductors where the dispersion relation lies within the semiconducting gap. Spin-excitons are found in the vicinity of magnetic quantum critical points in semiconductors, much the same as antiparamagnons are precursor fluctuations for quantum critical points in metals.Here we show that this concept of spin-exciton excitations can be extended to heavy-fermion semimetals and provides a natural explanation of the magnetic modes foun… Show more

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Cited by 5 publications
(2 citation statements)
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“…These materials are enabled by broken spatial or time inversion symmetries, and the large spin orbit interactions which collapses the conduction and valence bands within a limited section of the Brillouin zone where the conduction and valence bands cross and invert. Dirac, Weyl, nodal-line, and nested fermion semimetals have all been predicted theoretically and observed experimentally 6 11 . Weyl semimetals are particularly interesting since pairs of Weyl nodes with opposite chirality appear as monopole sources and sinks of Berry curvature 12 , 13 .…”
Section: Introductionmentioning
confidence: 90%
“…These materials are enabled by broken spatial or time inversion symmetries, and the large spin orbit interactions which collapses the conduction and valence bands within a limited section of the Brillouin zone where the conduction and valence bands cross and invert. Dirac, Weyl, nodal-line, and nested fermion semimetals have all been predicted theoretically and observed experimentally 6 11 . Weyl semimetals are particularly interesting since pairs of Weyl nodes with opposite chirality appear as monopole sources and sinks of Berry curvature 12 , 13 .…”
Section: Introductionmentioning
confidence: 90%
“…Supporting evidence for the exceptionally long lifetime of the spin-exciton has been provided by recent Raman scattering experiments [36] which see a q ∼ 0 feature at 16 meV with a width of 0.5 meV in an Al flux-grown SmB 6 sample at T = 15 K. The narrow line-width of the spin-exciton is caused by the absence of an electron-hole pair decay channel within the bulk hybridization gap. A shift of the peak from 13 meV in the bulk to 9 meV at the surface would indicate that the surface states are close to a quantum critical point [37]. The existence of large-amplitude, low-frequency spin-flip scattering at the surface would also result in the surface states not being completely protected from back-scattering and gives rise to a resonant peak in the low-temperature surface electronic density of states.…”
Section: Introductionmentioning
confidence: 99%