Representations of U(2∞) and the Value of the Fine Structure Constant

A relativistic quantum mechanics is formulated in which all of the interactions are in the four-momentum operator and Lorentz transformations are kinematic. Interactions are introduced through vertices, which are bilinear in fermion and antifermion creation and annihilation operators, and linear in...

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Збережено в:
Бібліографічні деталі
Опубліковано в: :Symmetry, Integrability and Geometry: Methods and Applications
Дата:2005
Автор: Klink, W.H.
Формат: Стаття
Мова:Англійська
Опубліковано: Інститут математики НАН України 2005
Онлайн доступ:https://nasplib.isofts.kiev.ua/handle/123456789/209332
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Назва журналу:Digital Library of Periodicals of National Academy of Sciences of Ukraine
Цитувати:Representations of U(2∞) and the Value of the Fine Structure Constant / W.H. Klink // Symmetry, Integrability and Geometry: Methods and Applications. — 2005. — Т. 1. — Бібліогр.: 7 назв. — англ.

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Digital Library of Periodicals of National Academy of Sciences of Ukraine
Опис
Резюме:A relativistic quantum mechanics is formulated in which all of the interactions are in the four-momentum operator and Lorentz transformations are kinematic. Interactions are introduced through vertices, which are bilinear in fermion and antifermion creation and annihilation operators, and linear in boson creation and annihilation operators. The fermion-antifermion operators generate a unitary Lie algebra, whose representations are fixed by a first-order Casimir operator (corresponding to baryon number or charge). Eigenvectors and eigenvalues of the four-momentum operator are analyzed, and exact solutions in the strong coupling limit are sketched. A simple model shows how the fine structure constant might be determined for the QED vertex.
ISSN:1815-0659