The S-matrix in quantum electrodynamics may be calculated alternatively from the Hamiltonian density −jμ(x)Aμ(x) and a Hamiltonian in which the Coulomb interaction of the charges and the interaction of the currents with the transverse field are separated. Both procedures are equivalent. Care must be taken, however, to define correctly the initial states, in particular the vacuum state. The definition of the vacuum state in both representations is discussed and the equivalence of the corresponding S-matrices is proven.</p
In our previous consideration, the so-called ambiguities of quantum field theory can be removed by t...
AbstractIn this note, we consider a Hamiltonian with ultraviolet and infrared cutoffs describing the...
Copyright © 2013 Walter Smilga. This is an open access article distributed under the Creative Common...
The formalism of quantum electrodynamics without subsidiary conditions was obtained in a relativisti...
Quantum electrodynamic bound states in strong electromagnetic fields are considered. It is shown tha...
The aim of this paper is to present a new approach to the formulation of. the quantum electrodynamic...
In quantum electrodynamics a classical part of the S-matrix is normally factored out in order to obt...
In this paper two things are done. (1) It is shown that a considerable simplification can be attaine...
A study of the connection between poles of the S-matrix and states of the Hamiltonian of non-relativ...
In this note, we consider an Hamiltonian, with ultraviolet and infrared cutoffs, describing the inte...
The new renonnalization procedure in quantum electrodynamics is presented in this paper. With this p...
The borderline of quantum electrodynamics and quantum optics offer spectacular results and problems ...
We consider an Hamiltonian with ultraviolet and infrared cutoffs, describing the interaction of rela...
In this classic text for advanced undergraduates and graduate students of physics, author Günter Sch...
The S matrix of e–e scattering has the structure of a projection operator that projects incoming sep...
In our previous consideration, the so-called ambiguities of quantum field theory can be removed by t...
AbstractIn this note, we consider a Hamiltonian with ultraviolet and infrared cutoffs describing the...
Copyright © 2013 Walter Smilga. This is an open access article distributed under the Creative Common...
The formalism of quantum electrodynamics without subsidiary conditions was obtained in a relativisti...
Quantum electrodynamic bound states in strong electromagnetic fields are considered. It is shown tha...
The aim of this paper is to present a new approach to the formulation of. the quantum electrodynamic...
In quantum electrodynamics a classical part of the S-matrix is normally factored out in order to obt...
In this paper two things are done. (1) It is shown that a considerable simplification can be attaine...
A study of the connection between poles of the S-matrix and states of the Hamiltonian of non-relativ...
In this note, we consider an Hamiltonian, with ultraviolet and infrared cutoffs, describing the inte...
The new renonnalization procedure in quantum electrodynamics is presented in this paper. With this p...
The borderline of quantum electrodynamics and quantum optics offer spectacular results and problems ...
We consider an Hamiltonian with ultraviolet and infrared cutoffs, describing the interaction of rela...
In this classic text for advanced undergraduates and graduate students of physics, author Günter Sch...
The S matrix of e–e scattering has the structure of a projection operator that projects incoming sep...
In our previous consideration, the so-called ambiguities of quantum field theory can be removed by t...
AbstractIn this note, we consider a Hamiltonian with ultraviolet and infrared cutoffs describing the...
Copyright © 2013 Walter Smilga. This is an open access article distributed under the Creative Common...