Gapped collective charge excitations and interlayer hopping in cuprate superconductors
Authors:
M. Hepting,
M. Bejas,
A. Nag,
H. Yamase,
N. Coppola,
D. Betto,
C. Falter,
M. Garcia-Fernandez,
S. Agrestini,
K. -J. Zhou,
M. Minola,
C. Sacco,
L. Maritato,
P. Orgiani,
H. I. Wei,
K. M. Shen,
D. G. Schlom,
A. Galdi,
A. Greco,
B. Keimer
Abstract:
We use resonant inelastic x-ray scattering (RIXS) to probe the propagation of plasmons in the electron-doped cuprate superconductor Sr$_{0.9}$La$_{0.1}$CuO$_2$ (SLCO). We detect a plasmon gap of $\sim$~120 meV at the two-dimensional Brillouin zone center, indicating that low-energy plasmons in SLCO are not strictly acoustic. The plasmon dispersion, including the gap, is accurately captured by laye…
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We use resonant inelastic x-ray scattering (RIXS) to probe the propagation of plasmons in the electron-doped cuprate superconductor Sr$_{0.9}$La$_{0.1}$CuO$_2$ (SLCO). We detect a plasmon gap of $\sim$~120 meV at the two-dimensional Brillouin zone center, indicating that low-energy plasmons in SLCO are not strictly acoustic. The plasmon dispersion, including the gap, is accurately captured by layered $t$-$J$-$V$ model calculations. A similar analysis performed on recent RIXS data from other cuprates suggests that the plasmon gap is generic and its size is related to the magnitude of the interlayer hopping $t_z$. Our work signifies the three-dimensionality of the charge dynamics in layered cuprates and provides a new method to determine $t_z$.
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Submitted 28 June, 2022;
originally announced June 2022.