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Weak and electromagnetic interactions
SummaryThe postulate of a «local connection» in a [3] charge space leads to the introduction of three spin one fields. One of these can be identified with the electro-magnetic field and the other twoExpand
Lepton Number as the Fourth Color
Universal strong, weak, and electromagnetic interactions of leptons and hadrons are generated by gauging a non-Abelian renormalizable anomaly-free subgroup of the fundamental symmetry structureExpand
d = 8 SUPERGRAVITY
Abstract SU(2) gauged N =2 supergravity in d =8 is constructed by generalized dimensional reduction of d =11 supergravity on SU(2) group manifold. The relation between the field equations of the d =8Expand
Chiral compactification on Minkowski × S2 of N = 2 Einstein-Maxwell supergravity in six dimensions
Abstract We show that the U(1) gauged Einstein-Maxwell supergravity in six dimensions, spontaneously compactifies on Minkowski × S 2 , with a monopole-valued Maxwell field on S 2 . The bosomicExpand
Electromagnetic and weak interactions
Abstract : In this note a synthesis is attempted between electromagnetism and weak interactions. No explanation is offered for the large boson mass value which results from one of the majorExpand
Super-gauge transformations
Abstract A systematic method for constructing Wess-Zumino supergauge transformations is exhibited.
Unified Lepton-Hadron Symmetry and a Gauge Theory of the Basic Interactions
An attempt is made to unify the fundamental hadrons and leptons into a common irreducible representation $F$ of the same symmetry group $G$ and to generate a gauge theory of strong, electromagnetic,Expand
Supergravities in diverse dimensions
This book is a collection of reprints on the structure of Poincare, anti-de Sitter and conformal supergravity theories in one to eleven dimensions, their anomalies and compactification. Each chapterExpand
Finite-component field representations of the conformal group
Abstract We review work done on realization of broken symmetry under the conformal group of space-time in the framework of finite-component field theory. Topics discussed include: Most generalExpand
On Kaluza-Klein theory
Abstract Assuming the compactification of 4 + K -dimensional space-time implied in Kaluza-Kleintype theories, we consider the case in which the internal manifold is a quotient space, G H . We developExpand
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