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Due to the small transition energy many body effects need to be included to accurately predict the spectral response peak position.
Hohenberg and Kohn [42] proved that the total energy of a system including that of the many body effects of electrons (exchange and correlation) in the presence of static external potential (for example, the atomic nuclei) is a unique function of the charge density.
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The discussed results shed light on the importance of many-body effects in systems of reduced dimensionality.
The possibility of using nanoelectromechanical systems as a simulation tool for quantum many-body effects is explored.
However, in the strongly interacting regime, these shifts became very small, reflecting the quantum unitarity limit and many-body effects.
Physically, lnΛ, known as the Coulomb logarithm, accounts for ion many-body effects such as repulsion and shielding within the one component plasma.
In this paper, we have devised a quantum simulator based on nanoelectromechanical systems, for analyzing the many-body effects in quantum systems.
In this context, it is very important to understand and control the many-body effects of competing heating processes in experiments.
This problem was first studied by Batista and Citrin[23] including the many-body effects arising from the macroscopic carrier density of the system.
Notably, many-body effects contribute more to the low-coverage adsorption systems than they do when the substrate is highly covered by the adsorbates.
The computational results are discussed in relation to multireference (MR) DFT, by which we treat the quantum many-body effects explicitly.
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