2021
DOI: 10.1103/physrevb.103.214505
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Enhancement of electron correlations in ion-gated FeSe film by in situ Seebeck and Hall measurements

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Cited by 7 publications
(3 citation statements)
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“…4 A ). The very large increase in observed in the thinnest -nm flake resembles the behavior of thin films of FeSe with lower RRR values ( 59 ). Recently, it was shown theoretically that the impurity scattering in FeSe can give rise to anisotropic scattering and anisotropy in resistivity ( 66 ).…”
Section: Discussionmentioning
confidence: 59%
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“…4 A ). The very large increase in observed in the thinnest -nm flake resembles the behavior of thin films of FeSe with lower RRR values ( 59 ). Recently, it was shown theoretically that the impurity scattering in FeSe can give rise to anisotropic scattering and anisotropy in resistivity ( 66 ).…”
Section: Discussionmentioning
confidence: 59%
“…Assuming that the effective masses of heavy electrons are the same for the bulk and thin flakes, then the changes in mobilities between electron and hole carriers could reflect an anisotropy in scattering (classical scattering time being ps for electrons and 1.8 ps for holes). Interestingly, the effective mass extracted from ARPES studies is much smaller, , for a single momentum direction ( 7 , 13 ), and it can be enhanced in thin films and flakes of FeSe up to , both using K-dosing of FeSe ( 58 ) and ionic liquid gating ( 59 ). Orbitally dependent band shifts and renormalizations were detected previously in FeSe, with the dominant d xy hole band being the most renormalized by a factor of 8, as compared with a factor 2.5 to 3.5 for the d xz and d yz orbitals ( 2 , 7 ).…”
Section: Discussionmentioning
confidence: 99%
“…It is worth pointing out that the temperature of ∼52 K at which the resistance deviates from the linear extrapolation of the normal state agrees well with a \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{upgreek} \usepackage{mathrsfs} \setlength{\oddsidemargin}{-69pt} \begin{document} $T_{\mathrm{c}}^{{\mathrm{on}}}$\end{document} of ∼50 K in FeSe–EDLT, supporting that the disorder still dominates the wide transition in the monolayer FeSe on the δ-doped STO(001). Moreover, the EDLT doping could enhance electron correlation compared with the monolayer FeSe (3.4 vs. 2.7 m e , where m e is the free electron mass) [ 56 , 57 ]. Between T p of ∼65–83 K and \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{upgreek} \usepackage{mathrsfs} \setlength{\oddsidemargin}{-69pt} \begin{document} $T_{\mathrm{c}}^{{\mathrm{on}}}$\end{document} of ∼50 K, whether the pseudogap state or BKT physics dominates remains unsolved.…”
Section: Discussionmentioning
confidence: 99%