{ "id": "2408.03970", "version": "v1", "published": "2024-08-06T23:26:28.000Z", "updated": "2024-08-06T23:26:28.000Z", "title": "Thermal quasi-particle theory", "authors": [ "So Hirata" ], "categories": [ "cond-mat.stat-mech", "physics.chem-ph", "physics.comp-ph" ], "abstract": "The widely used thermal Hartree-Fock (HF) theory is generalized to include the effect of electron correlation while maintaining its quasi-independent-particle framework. An electron-correlated internal energy (or grand potential) is defined by the second-order finite-temperature many-body perturbation theory (MBPT), which then dictates the corresponding thermal orbital (quasi-particle) energies in such a way that all thermodynamic relations are obeyed. The associated density matrix is of the one-electron type, whose diagonal elements take the form of the Fermi-Dirac distribution functions, when the grand potential is minimized. The formulas for the entropy and chemical potential are unchanged from those of Fermi-Dirac or thermal HF theory. The theory thus postulates a finite-temperature extension of the second-order Dyson self-energy of one-particle many-body Green's function theory and can be viewed as a second-order, diagonal, frequency-independent, thermal inverse Dyson equation. At low temperature, the theory approaches finite-temperature MBPT of the same order, but it outperforms the latter at intermediate temperature by including additional electron-correlation effects through orbital energies. A physical meaning of these thermal orbital energies (including that of thermal HF orbital energies, which has been elusive) is proposed.", "revisions": [ { "version": "v1", "updated": "2024-08-06T23:26:28.000Z" } ], "analyses": { "keywords": [ "thermal quasi-particle theory", "second-order finite-temperature many-body perturbation theory", "one-particle many-body greens function theory", "grand potential", "thermal hf orbital energies" ], "note": { "typesetting": "TeX", "pages": 0, "language": "en", "license": "arXiv", "status": "editable" } } }