Density-matrix renormalization group study of optical conductivity of the Mott insulator for two-dimensional clusters
arXiv:2109.06226 · doi:10.1103/PhysRevB.104.205123
Abstract
The real part of optical conductivity of the Mott insulators has a large amount of information on how spin and charge degrees of freedom interact with each other. By using the time-dependent density-matrix renormalization group, we study of the two-dimensional Hubbard model on a square lattice at half filling. We find an excitonic peak at the Mott-gap edge of not only for the two-dimensional square lattice but also for two- and four-leg ladders. For the square lattice, however, we do not clearly find a gap between an excitonic peak and continuum band, which indicates that a bound state is not well defined. The emergence of an excitonic peak in implies the formation of a spin polaron. Examining the dependence of on the on-site Coulomb interaction and next-nearest neighbor hoppings, we confirm that an excitonic peak is generated from a magnetic effect. Electron scattering due to an electron-phonon interaction is expected to easily suppress an excitonic peak since spectral width of an excitonic peak is very narrow. Introducing a large broadening in by modeling the electron-phonon coupling present in LaCuO and NdCuO, we obtain comparable with experiments.
arXiv comment10 pages, 8 figures
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- Many-body effects on high-harmonic generation in Hubbard ladders
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- Controlling inversion and time-reversal symmetries by subcycle pulses in the one-dimensional extended Hubbard model
- Observation of excitons bound by antiferromagnetic correlations
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- Exciton-spin interactions in antiferromagnetic charge-transfer insulators
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