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Evolution of the low temperature Fermi surface of superconducting FeSe1−xSx across a nematic phase transition

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Figure

Fig. 1Quantum oscillations in superconducting single crystals of FeSesignalwith their positions indicated by vertical arrows.1−xSx
Fig. 2Quasiparticle effective masses and the angular dependence of quantum oscillations
Fig. 3Evolution of the electronic properties of FeSeIn1−xSx. a Phase diagram of FeSe1−xSx as a function of sulphur substitution, x indicating thesuppression of the nematic phase (Ts, solid triangles) and the presence of a small dome of superconductivity (T

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