Fig. 4: Plasmon dispersion along the momentum q parallel to the layers for several q perpendicular to the layers (squares) together with calculations within the framework of the Fetter model (solid lines). | Nature Communications

Fig. 4: Plasmon dispersion along the momentum q parallel to the layers for several q perpendicular to the layers (squares) together with calculations within the framework of the Fetter model (solid lines).

From: Optical and acoustic plasmons in the layered material Sr2RuO4

Fig. 4

The q values 0, 0.1, 0.2, 0.3, and 0.4 Å−1 are marked by purple, blue, green, yellow, and red color symbols, respectively (see Fig. 3). We have added also the data from the optical plasmon dispersion derived in our previous publication (dark purple diamonds)38. The horizontal error bars originate from the finite momentum resolution while the vertical ones are related to the finite spectral resolution of the EEL spectrometer (the fitting error is small in comparison). The region marked in gray corresponds to the susceptibility χ0 calculated from a tight binding band structure (see below and Methods). The excitations in the continuum range are marked by open symbols. The colored solid (dashed) curves correspond to theoretical data considering (neglecting) finite momentum resolution, i.e., integration within the EEL collection aperture.

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