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dc.contributor.authorBartlett, J.M.
dc.contributor.authorSteppke, A.
dc.contributor.authorHosoi, S.
dc.contributor.authorNoad, H.
dc.contributor.authorPark, J.
dc.contributor.authorTimm, C.
dc.contributor.authorShibauchi, T.
dc.contributor.authorMackenzie, A.P.
dc.contributor.authorHicks, C.W.
dc.date.accessioned2021-06-15T09:05:44Z
dc.date.available2021-06-15T09:05:44Z
dc.date.issued2021-05-19
dc.identifier274588859
dc.identifiere2fdd0bd-7b09-44d2-af42-f05d31f4729f
dc.identifier85106500633
dc.identifier000655928900001
dc.identifier.citationBartlett , J M , Steppke , A , Hosoi , S , Noad , H , Park , J , Timm , C , Shibauchi , T , Mackenzie , A P & Hicks , C W 2021 , ' Relationship between transport anisotropy and nematicity in FeSe ' , Physical Review X , vol. 11 , no. 2 , 021038 . https://doi.org/10.1103/PhysRevX.11.021038en
dc.identifier.issn2160-3308
dc.identifier.otherRIS: urn:79C7E8414C99C813E6FC1C8CEBF0F107
dc.identifier.urihttps://hdl.handle.net/10023/23361
dc.descriptionWe thank the Max Planck Society for financial support. C. W. H., A. P. M., and C. T. acknowledge support by the DFG (DE) through the Collaborative Research Centre SFB 1143 (Projects C09 and A04). C. T. acknowledges support by the DFG (DE) through the Cluster of Excellence on Complexity and Topology in Quantum Matter ct.qmat (EXC 2147). Work in Japan was supported by Grants-in-Aid for Scientific Research (KAKENHI) (No. JP19H00649 and No. JP18H05227), and Grant-in-Aid for Scientific Research on innovative areas “Quantum Liquid Crystals” (No. JP19H05824 and No. JP20H05162) from Japan Society for the Promotion of Science (JSPS).en
dc.description.abstractThe mechanism behind the nematicity of FeSe is not known. Through elastoresitivity measurements it has been shown to be an electronic instability. However, thus far measurements have extended only to small strains, where the response is linear. Here, we apply large elastic strains to FeSe and perform two types of measurement. (1) Using applied strain to control twinning, the nematic resistive anisotropy at temperatures below the nematic transition temperature Ts is determined. (2) Resistive anisotropy is measured as nematicity is induced through applied strain at fixed temperature above Ts. In both cases, as nematicity strengthens, the resistive anisotropy peaks at about 7%, then decreases. Below ≈40  K, the nematic resistive anisotropy changes sign. We discuss possible implications of this behavior for theories of nematicity. In addition, we report the following. (1) Under experimentally accessible conditions with bulk crystals, stress, rather than strain, is the conjugate field to the nematicity of FeSe. (2) At low temperatures the twin boundary resistance is ∼10% of the sample resistance, and must be properly subtracted to extract intrinsic resistivities. (3) Biaxial in-plane compression increases both in-plane resistivity and the superconducting critical temperature Tc, consistent with a strong role of the yz orbital in the electronic correlations.
dc.format.extent19
dc.format.extent2533788
dc.language.isoeng
dc.relation.ispartofPhysical Review Xen
dc.subjectCondensed matter physicsen
dc.subjectStrongly correlated materialsen
dc.subjectSuperconductivityen
dc.subjectQC Physicsen
dc.subjectTK Electrical engineering. Electronics Nuclear engineeringen
dc.subjectT-NDASen
dc.subject.lccQCen
dc.subject.lccTKen
dc.titleRelationship between transport anisotropy and nematicity in FeSeen
dc.typeJournal articleen
dc.contributor.institutionUniversity of St Andrews. School of Physics and Astronomyen
dc.contributor.institutionUniversity of St Andrews. Condensed Matter Physicsen
dc.identifier.doi10.1103/PhysRevX.11.021038
dc.description.statusPeer revieweden


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