Towards a Quantum Fluid Theory of Correlated Many-Fermion Systems from First Principles
arXiv:2103.08523 · doi:10.21468/SciPostPhys.12.2.062
Abstract
Correlated many-fermion systems emerge in a broad range of phenomena in warm dense matter, plasmonics, and ultracold atoms. Quantum hydrodynamics (QHD) complements common first-principles methods for many-fermion systems and enables simulations at larger length and longer time scales. While the quantum Bohm potential is central to QHD, we illustrate its failure for strong perturbations. We extend QHD to this regime by utilizing the many-fermion quantum Bohm potential. This opens up the path to more accurate simulations in strongly perturbed warm dense matter, inhomogeneous quantum plasmas, and on nano-structure surfaces at scales unattainable with first-principles algorithms. The many-fermion quantum Bohm potential might also have important astrophysical applications in developing conformal-invariant cosmologies.
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- Linear-response time-dependent density functional theory approach to warm dense matter with adiabatic exchange--correlation kernels
- Non-empirical mixing coefficient for hybrid XC functionals from analysis of the XC kernel
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- Averaging over atom snapshots in linear-response TDDFT of disordered systems: A case study of warm dense hydrogen
- Imposing Correct Jellium Response Is Key to Predict the Density Response by Orbital-Free DFT
- Development of a new quantum trajectory molecular dynamics framework
- Energy response and spatial alignment of the perturbed electron gas
- Ion core effect on transport characteristics in warm dense matter