On the exact mean-field description of continuous quantum systems in equilibrium

DOI10.1016/0378-4371(83)90021-3zbMath0533.70013OpenAlexW4235487882MaRDI QIDQ789909

J. Maćkowiak

Publication date: 1983

Published in: Physica A (Search for Journal in Brave)

Full work available at URL: https://doi.org/10.1016/0378-4371(83)90021-3

zbMATH Keywords

thermodynamic limitFeynman-Kac formulasaddle point methodmean field approximationfree energy densityBogolyubov inequalityBoltzmann, Fermi-Dirac and Bose-Einstein statisticsquantum continuous systemseparable 2-body interactions

Mathematics Subject Classification ID

General aerodynamics and subsonic flows (76G25) Quantum equilibrium statistical mechanics (general) (82B10) Lattice systems (Ising, dimer, Potts, etc.) and systems on graphs arising in equilibrium statistical mechanics (82B20)

Cites Work

• On uniqueness of KmMS states of one-dimensional quantum lattice systems
• The classical limit of quantum spin systems
• Some remarks on the ground state of infinite systems in statistical mechanics
• Equilibrium states for mean field models
• Feynman Integrals and the Schrödinger Equation
• Statistical Theory of Equations of State and Phase Transitions. I. Theory of Condensation
• Theory of Superconductivity
• Unnamed Item
• Unnamed Item
• Unnamed Item
• Unnamed Item

This page was built for publication: On the exact mean-field description of continuous quantum systems in equilibrium