Add to ORKGAbstract. Let N ^ denote the maximum number of electrons that can be bound to an atom of nuclear charge z, in the Thomas-Fermi-von Weizsacker theory. It is proved that N^ cannot exceed z by more than one, and thus this theory is in agreement with experimental facts about real atoms. A similar result is proved for molecules, i.e. N ^ cannot exceed the total nuclear charge by more than the number of atoms in the molecule
Recently[1, 2], we have studied the role of electron correlation in model atoms at weak binding cond...
It was proved by Benguria and Lieb that for an atom where the ‘electrons’ do not satisfy the exclusi...
Let N(Z) denote the number of electrons that a nucleus of charge Z binds in nonrelativistic quantum ...
We prove that in Thomas–Fermi–Dirac–von Weizsäcker theory, a nucleus of charge Z > 0 can bind at mos...
We study the Thomas-Fermi-von Weizsäcker theory of atoms and molecules. The main result is to prove ...
We consider an atom described by Müller theory, which is similar to Hartree–Fock theory, but with a ...
We study the ionization problem in the Thomas-Fermi-Dirac-von Weizsäcker theory for atoms and molecu...
Let N(Z) denote the number of electrons which a nucleus of charge Z can bind in non-relativistic qua...
We prove that in Thomas–Fermi–Dirac–von Weizsäcker theory, a nucleus of charge Z > 0 can bind at ...
As the nuclear charge Z is continuously decreased an N-electron atom undergoes a binding-unbinding t...
AbstractWe place the Thomas-Fermi model of the quantum theory of atoms, molecules, and solids on a f...
We prove the ionization conjecture within the Hartree-Fock theory of atoms. More precisely, we prove...
AbstractIn this paper, we prove that the energy of an atom with nuclear charge Z is greater than − C...
In this paper, we investigate the maximum number of electrons that can be bound to a system of nucle...
Abstract. We consider the zero mass limit of a relativistic Thomas–Fermi– Weizsäcker model of atoms...
Recently[1, 2], we have studied the role of electron correlation in model atoms at weak binding cond...
It was proved by Benguria and Lieb that for an atom where the ‘electrons’ do not satisfy the exclusi...
Let N(Z) denote the number of electrons that a nucleus of charge Z binds in nonrelativistic quantum ...
We prove that in Thomas–Fermi–Dirac–von Weizsäcker theory, a nucleus of charge Z > 0 can bind at mos...
We study the Thomas-Fermi-von Weizsäcker theory of atoms and molecules. The main result is to prove ...
We consider an atom described by Müller theory, which is similar to Hartree–Fock theory, but with a ...
We study the ionization problem in the Thomas-Fermi-Dirac-von Weizsäcker theory for atoms and molecu...
Let N(Z) denote the number of electrons which a nucleus of charge Z can bind in non-relativistic qua...
We prove that in Thomas–Fermi–Dirac–von Weizsäcker theory, a nucleus of charge Z > 0 can bind at ...
As the nuclear charge Z is continuously decreased an N-electron atom undergoes a binding-unbinding t...
AbstractWe place the Thomas-Fermi model of the quantum theory of atoms, molecules, and solids on a f...
We prove the ionization conjecture within the Hartree-Fock theory of atoms. More precisely, we prove...
AbstractIn this paper, we prove that the energy of an atom with nuclear charge Z is greater than − C...
In this paper, we investigate the maximum number of electrons that can be bound to a system of nucle...
Abstract. We consider the zero mass limit of a relativistic Thomas–Fermi– Weizsäcker model of atoms...
Recently[1, 2], we have studied the role of electron correlation in model atoms at weak binding cond...
It was proved by Benguria and Lieb that for an atom where the ‘electrons’ do not satisfy the exclusi...
Let N(Z) denote the number of electrons that a nucleus of charge Z binds in nonrelativistic quantum ...