Ground State and Charge Renormalization in a Nonlinear Model of Relativistic Atoms
arXiv:0712.2911 · doi:10.1007/s00220-008-0660-9
Abstract
We study the reduced Bogoliubov-Dirac-Fock (BDF) energy which allows to describe relativistic electrons interacting with the Dirac sea, in an external electrostatic potential. The model can be seen as a mean-field approximation of Quantum Electrodynamics (QED) where photons and the so-called exchange term are neglected. A state of the system is described by its one-body density matrix, an infinite rank self-adjoint operator which is a compact perturbation of the negative spectral projector of the free Dirac operator (the Dirac sea). We study the minimization of the reduced BDF energy under a charge constraint. We prove the existence of minimizers for a large range of values of the charge, and any positive value of the coupling constant . Our result covers neutral and positively charged molecules, provided that the positive charge is not large enough to create electron-positron pairs. We also prove that the density of any minimizer is an function and compute the effective charge of the system, recovering the usual renormalization of charge: the physical coupling constant is related to by the formula , where is the ultraviolet cut-off. We eventually prove an estimate on the highest number of electrons which can be bound by a nucleus of charge . In the nonrelativistic limit, we obtain that this number is , recovering a result of Lieb. This work is based on a series of papers by Hainzl, Lewin, Sere and Solovej on the mean-field approximation of no-photon QED.
arXiv comment37 pages, 1 figure
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- The Pauli-Villars regularised free energy of Dirac's vacuum in purely magnetic fields
- The positronium in a mean-field approximation of quantum electrodynamics
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