Exact first-order density matrix for a d-dimensional harmonically confined Fermi gas at finite temperature
arXiv:cond-mat/0306320 · doi:10.1103/PhysRevA.68.033601
Abstract
We present an exact closed form expression for the {\em finite temperature} first-order density matrix of a harmonically trapped ideal Fermi gas in any dimension. This constitutes a much sought after generalization of the recent results in the literature, where exact expressions have been limited to quantities derived from the {\em diagonal} first-order density matrix. We compare our exact results with the Thomas-Fermi approximation (TFA) and demonstrate numerically that the TFA provides an excellent description of the first-order density matrix in the large-N limit. As an interesting application, we derive a closed form expression for the finite temperature Hartree-Fock exchange energy of a two-dimensional parabolically confined quantum dot. We numerically test this exact result against the 2D TF exchange functional, and comment on the applicability of the local-density approximation (LDA) to the exchange energy of an inhomogeneous 2D Fermi gas.
12 pages, 3 figures included in the text, RevTeX4. Text before Eq.(25) corrected. Additional equation following Eq.(25) has been added
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- Ideal Fermi gases in harmonic oscillator potential traps
- Exact results for a charged, harmonically trapped quantum gas at arbitrary temperature and magnetic field strength
- Harmonically trapped jellium
- Finite temperature analytical results for a harmonically confined gas obeying exclusion statistics in -dimensions
- A manifestly Hermitian semiclassical expansion for the one-particle density matrix of a two-dimensional Fermi gas
- The Classical-Map Hyper-Netted-Chain (CHNC) technique for inhomogeneous electron systems. Application to quantum dots
- Evaluation of inverse integral transforms for undergraduate physics students
- Preserving the Hermiticity of the One-Body Density Matrix for a Non-Interacting Fermi Gas