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In-plane anisotropy of transport coefficients in electronic nematic states: Universal origin of nematicity in Fe-based superconductors

Seiichiro Onari, Hiroshi Kontani

DOI 10.1103/PhysRevB.96.094527 · Physical Review B

T1

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Abstract

The origin of the electronic nematicity and its remarkable material dependence are famous longstanding unsolved issues in Fe-based superconductors. To attack these issues, we focus on the in-plane anisotropy of the resistivity: In the nematic state in FeSe, the relation ρx>ρy holds, where ρx(y) is the resistivity along the longer (shorter) Fe-Fe axis. In contrast, the opposite anisotropy ρx<ρy is realized in other undoped Fe-based superconductors. Such nontrivial material dependence is naturally explained in terms of the strongly orbital-dependent inelastic quasiparticle scattering realized in the orbital-ordered state. The opposite anisotropy between FeSe (ρx>ρy) and other undoped compounds (ρx<ρy) reflects the difference in the number of hole pockets. We also explain the large in-plane anisotropy of the thermoelectric power in the nematic state.

Source-reported materials — not catalogue approval

FormulaReported Tc (K)Pressure (GPa)Type
FeSe

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—Pressure not reportedunknown
Ba(Fe1-xCox)2As2

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—Pressure not reportedunknown
Ba(As1-xPx)2

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—Pressure not reportedunknown
EuFe2(As1-xPx)2

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—Pressure not reportedunknown
BaFe2As2

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—Pressure not reportedunknown
LaFeAsO

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—Pressure not reportedunknown

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