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Magnetic phases of skyrmion-hosting GaV\\(_4\\)S\\(_{8-y}\\)Se\\(_{y}\\) (\\(y = 0, 2, 4, 8\\)) probed with muon spectroscopy
Magnetic phases of skyrmion-hosting GaV\\(_4\\)S\\(_{8-y}\\)Se\\(_{y}\\) (\\(y = 0, 2, 4, 8\\)) probed with muon spectroscopy
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Magnetic phases of skyrmion-hosting GaV\\(_4\\)S\\(_{8-y}\\)Se\\(_{y}\\) (\\(y = 0, 2, 4, 8\\)) probed with muon spectroscopy
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Magnetic phases of skyrmion-hosting GaV\\(_4\\)S\\(_{8-y}\\)Se\\(_{y}\\) (\\(y = 0, 2, 4, 8\\)) probed with muon spectroscopy
Magnetic phases of skyrmion-hosting GaV\\(_4\\)S\\(_{8-y}\\)Se\\(_{y}\\) (\\(y = 0, 2, 4, 8\\)) probed with muon spectroscopy

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Magnetic phases of skyrmion-hosting GaV\\(_4\\)S\\(_{8-y}\\)Se\\(_{y}\\) (\\(y = 0, 2, 4, 8\\)) probed with muon spectroscopy
Magnetic phases of skyrmion-hosting GaV\\(_4\\)S\\(_{8-y}\\)Se\\(_{y}\\) (\\(y = 0, 2, 4, 8\\)) probed with muon spectroscopy
Paper

Magnetic phases of skyrmion-hosting GaV\\(_4\\)S\\(_{8-y}\\)Se\\(_{y}\\) (\\(y = 0, 2, 4, 8\\)) probed with muon spectroscopy

2018
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Overview
We present the results of a muon-spin spectroscopy investigation of GaV\\(_4\\)S\\(_{8-y}\\)Se\\(_{y}\\) with \\(y=0, 2, 4\\) and 8. Zero-field measurements suggest that GaV\\(_{4}\\)Se\\(_{8}\\) and GaV\\(_{4}\\)S\\(_{8}\\) have distinct magnetic ground states, with the latter material showing an anomalous temperature-dependence of the local magnetic field. It is not possible to evolve the magnetic state continuously between these two systems, with the intermediate \\(y=2\\) and \\(4\\) materials showing glassy magnetic behaviour at low temperature. The skyrmion lattice (SkL) phase is evident in the \\(y=0\\) and 8 materials through an enhanced response of the muon-spin relaxation to the emergent dynamics that accompany the SkL. For our polycrystalline samples of GaV\\(_4\\)Se\\(_{8}\\), this enhanced dynamic response is confined to a smaller region of the magnetic field-temperature phase diagram than the previous reports of the SkL in single crystals.