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Updated: May 28, 2025

Excitonic Hamiltonians for Calculating Optical Absorption Spectra and Optoelectronic Properties of Molecular Aggregates and Solids
Published on: May 27, 2020
Short-Range Excitonic Phenomena in Low-Density Metals.
Jaakko Koskelo1,2, Lucia Reining1,2, Matteo Gatti1,2,3
1Institut Polytechnique de Paris, LSI, CNRS, CEA/DRF/IRAMIS, École Polytechnique, F-91120 Palaiseau, France.
Excitonic effects, typically weak in metals, emerge in low-density electron gases due to reduced screening. These findings reveal novel low-energy collective modes with excitonic properties.
Area of Science:
- Condensed matter physics
- Quantum mechanics
Background:
- Excitonic effects are generally considered weak in metals due to strong Coulomb screening.
- Recent theoretical suggestions point to the possibility of low-energy excitonic collective modes in the homogeneous electron gas.
Purpose of the Study:
- To investigate the existence and nature of low-energy excitonic collective modes in the low-density homogeneous electron gas.
- To explore the role of reduced screening and electron-hole correlations in these phenomena.
Main Methods:
- Utilizing the Bethe-Salpeter equation (BSE) for ab initio calculations.
- Addressing and overcoming the self-polarization error in standard BSE approximations.
- Analyzing the electron-hole wave function to determine excitonic character.
Main Results:
- Confirmed the emergence of low-energy collective modes in the low-density electron gas.
- Demonstrated that reduced screening at short distances facilitates these excitonic effects.
- Observed strong, anisotropic electron-hole correlations characteristic of excitonic behavior.
- Showcased the capability of the adiabatic local density approximation to capture these effects.
Conclusions:
- Low-density electron gases can exhibit significant excitonic effects, challenging conventional understanding.
- These findings highlight the importance of short-distance electron-hole interactions and reduced screening.
- The identified exotic regime may be observable in doped semiconductors and interfaces.
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