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Quantum-Electrodynamical Density-Functional Theory Exemplified by the Quantum Rabi Model
Vebjørn H. Bakkestuen +5 more
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METHOD OF EIGENFUNCTIONS AND MASS OPERATOR IN QUANTUM ELECTRODYNAMICS OF A CONSTANT FIELD
V. I. Ritus
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Topological quantum electrodynamics in synthetic non-Abelian gauge fields
Anonymous
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Quantum electrodynamic description of the neutral hydrogen molecule ionization [PDF]
Miao Hui-hui
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On the Existence of Quantum Electrodynamics
Physical Review Letters, 1988A partir d'une perspective intuitive du groupe de renormalisation, on explique comment l'«effondrement de la fonction d'onde», dans l'electrodynamique quantique gele, conduit a la renormalisation de la constante de couplage et un point fixe stable ultraviolet en interaction. Un developpement diagrammatique en Nf(le nombre d'especes de fermions) suggere
, Kogut, , Dagotto, , Kocic
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Development of quantum electrodynamics
Physics Today, 1966IN 1932, when I started my research career as an assistant to Nishina, Dirac published a paper in the Proceedings of the Royal Society, London. In this paper, he discussed the formulation of relativistic quantum mechanics, especially that of electrons interacting with the electromagnetic field.
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On the Renormalization of Quantum Electrodynamics
Proceedings of the Physical Society. Section A, 1951The subtraction procedure of Dyson is modified in order to eliminate a certain difficulty in the renormalization programme, namely the so-called `b' divergencies. The conclusions of Dyson concerning the finiteness of the renormalized S matrix are confirmed.
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Mathematical Proceedings of the Cambridge Philosophical Society, 1939
It is shown in this paper and the preceding one that two separate forms of theory can be developed in which a “finite size” is attributed to a charged particle by means of its interaction with the radiation field. The region attributed in this way to the particle is four dimensional and is determined in such a manner that the usual difficulties with ...
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It is shown in this paper and the preceding one that two separate forms of theory can be developed in which a “finite size” is attributed to a charged particle by means of its interaction with the radiation field. The region attributed in this way to the particle is four dimensional and is determined in such a manner that the usual difficulties with ...
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