Fig. 4: Phonon eigenmodes and microscopic mechanism of electronic band modulation. | Nature Communications

Fig. 4: Phonon eigenmodes and microscopic mechanism of electronic band modulation.

From: Strong electron-phonon coupling driven pseudogap modulation and density-wave fluctuations in a correlated polar metal

Fig. 4

a Illustration of the Ru and O atoms, bond lengths between oxygens and the bond angle of O-Ru-O. b The illustrations of the eigen mode of B2P, and c that of B2M. d The averaged ratio of RuO6 octahedra cage apical Ru-O bond length (\({d}_{\perp }\)) over in-plane bond length (\({d}_{\parallel }\)) modulated by two phonons. e Averaged in-plane bond angle (\(\theta\)) modulated by the two phonons.  (see Supplementary Figs. 15 for phonon modulated bond length and angles in two types of RuO6f The density of states plots of the AFM-b ground state (middle) and the modulated AFM-b state by B2M (top) and B2P (bottom). g Correlation between octahedra distortion (\({d}_{\perp }\)/\({d}_{\parallel }\)), in plane bond angle (\(\theta\)) and the density of states near the Fermi surface. The lines are guides to the eye.

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