Constraints of reduced density-matrix functional theory for the two-dimensional homogeneous electron gas
arXiv:1105.2473 · doi:10.1103/PhysRevB.84.035104
Abstract
Reduced density-matrix functional theory (RDMFT) has become an appealing alternative to density-functional theory to describe electronic properties of highly-correlated systems. Here we derive exact conditions for the suitability of RDMFT to describe the two-dimensional homogeneous electron gas, which is the base system for, e.g., semiconductor quantum dots and quantum Hall devices. Following the method of Cioslowski and Pernal [J. Chem. Phys. {\bf 111}, 3396 (1999)] we focus on the properties of power functionals of the form for the scaling function in the exchange-correlation energy. We show that in order to have stable and analytic solutions, and for to satisfy the homogeneous scaling constraint, the power is restricted to . Applying a reasonable ansatz for the momentum distribution and the lower bound for the exchange-correlation energy tightens the physical regime further to .
References in corpus (10)
- Reduced Density Matrix Functional for Many-Electron Systems
- Combining Density Functional Theory and Density Matrix Functional Theory
- Collapse of the Electron Gas to Two Dimensions in Density Functional Theory
- Lower Bounds on the Exchange-Correlation Energy in Reduced Dimensions
- Dimensional crossover of the exchange-correlation energy at the semilocal level
- Interaction-Induced Spin Polarization in Quantum Dots
- Density gradients for the exchange energy of electrons in two dimensions
- Parameter-free density functional for the correlation energy in two dimensions
- Reduced density-matrix functional theory in quantum Hall systems
- Laplacian-level density functionals for the exchange-correlation energy of low-dimensional nanostructures