Existence of Atoms and Molecules in the Mean-Field Approximation of No-Photon Quantum Electrodynamics

被引:26
作者
Hainzl, Christian [1 ]
Lewin, Mathieu [2 ,3 ]
Sere, Eric [4 ]
机构
[1] Univ Alabama Birmingham, Dept Math, Birmingham, AL 35294 USA
[2] Univ Cergy Pontoise, CNRS, F-95302 Cergy Pontoise, France
[3] Univ Cergy Pontoise, Dept Math, CNRS, UMR 8088, F-95302 Cergy Pontoise, France
[4] Univ Paris 09, CEREMADE, CNRS, UMR 7534, F-75775 Paris 16, France
关键词
CONCENTRATION-COMPACTNESS PRINCIPLE; DIRAC-FOCK EQUATIONS; VARIATIONAL PRINCIPLE; POLARIZED VACUUM; ELECTRONS; ENERGY; PAIR; STABILITY; CALCULUS;
D O I
10.1007/s00205-008-0144-2
中图分类号
O29 [应用数学];
学科分类号
070104 ;
摘要
The Bogoliubov-Dirac-Fock (BDF) model is the mean-field approximation of no-photon quantum electrodynamics. The present paper is devoted to the study of the minimization of the BDF energy functional under a charge constraint. An associated minimizer, if it exists, will usually represent the ground state of a system of N electrons interacting with the Dirac sea, in an external electrostatic field generated by one or several fixed nuclei. We prove that such a minimizer exists when a binding (HVZ-type) condition holds. We also derive, study and interpret the equation satisfied by such a minimizer. Finally, we provide two regimes in which the binding condition is fulfilled, obtaining the existence of a minimizer in these cases. The first is the weak coupling regime for which the coupling constant alpha is small whereas alpha Z and the particle number N are fixed. The second is the non-relativistic regime in which the speed of light tends to infinity (or equivalently alpha tends to zero) and Z, N are fixed. We also prove that the electronic solution converges in the non-relativistic limit towards a Hartree-Fock ground state.
引用
收藏
页码:453 / 499
页数:47
相关论文
共 64 条
[1]   The positive electron [J].
Anderson, CD .
PHYSICAL REVIEW, 1933, 43 (06) :491-494
[2]  
[Anonymous], 9 U CAL
[3]   THE INDEX OF A PAIR OF PROJECTIONS [J].
AVRON, J ;
SEILER, R ;
SIMON, B .
JOURNAL OF FUNCTIONAL ANALYSIS, 1994, 120 (01) :220-237
[4]   THERE ARE NO UNFILLED SHELLS IN UNRESTRICTED HARTREE-FOCK THEORY [J].
BACH, V ;
LIEB, EH ;
LOSS, M ;
SOLOVEJ, JP .
PHYSICAL REVIEW LETTERS, 1994, 72 (19) :2981-2983
[5]   On the stability of the relativistic electron-positron field [J].
Bach, V ;
Barbaroux, JM ;
Helffer, B ;
Siedentop, H .
COMMUNICATIONS IN MATHEMATICAL PHYSICS, 1999, 201 (02) :445-460
[6]   GENERALIZED HARTREE-FOCK THEORY AND THE HUBBARD-MODEL [J].
BACH, V ;
LIEB, EH ;
SOLOVEJ, JP .
JOURNAL OF STATISTICAL PHYSICS, 1994, 76 (1-2) :3-89
[7]   ERROR BOUND FOR THE HARTREE-FOCK ENERGY OF ATOMS AND MOLECULES [J].
BACH, V .
COMMUNICATIONS IN MATHEMATICAL PHYSICS, 1992, 147 (03) :527-548
[8]  
Bhatia Rajendra, 1997, Matrix Analysis: Graduate Texts in Mathematics, V169
[9]   A SMOOTH VARIATIONAL PRINCIPLE WITH APPLICATIONS TO SUBDIFFERENTIABILITY AND TO DIFFERENTIABILITY OF CONVEX-FUNCTIONS [J].
BORWEIN, JM ;
PREISS, D .
TRANSACTIONS OF THE AMERICAN MATHEMATICAL SOCIETY, 1987, 303 (02) :517-527
[10]   FROM QUANTUM ELECTRODYNAMICS TO MEAN-FIELD THEORY .1. THE BOGOLIUBOV-DIRAC-FOCK FORMALISM [J].
CHAIX, P ;
IRACANE, D .
JOURNAL OF PHYSICS B-ATOMIC MOLECULAR AND OPTICAL PHYSICS, 1989, 22 (23) :3791-3814