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- W2963757816 abstract "The construction of a gauge field theory for elementary particles usually starts by promoting global invariance of the matter action to a local one, this in turn implying the introduction of gauge fields. We present here a procedure that runs the other way: starting from the action for gauge fields, matter is gauge invariantly coupled on the basis of Lorentz invariance and charge conservation. This natural approach prevents using the concept of particles separated from gauge fields that mediate interactions. Gauge invariance was introduced by H. Weyl (1) in 1919 in an attempt of unifying electrodynamics and general relativity. In his original proposal, gauging meant a space dependent change in the space-time unit of length together with the rescaling of the compensating or connection fields, the gauge potentials. Weyl's original proposal was incorrect but, nevertheless, the concept of gauge invariance survived as a central symmetry of Maxwell equations, extremely useful in the development of electrodynamics, particularly at the quantum level. At present, electromagnetic interactions of matter mediated by photons can be understood arising from the requirement of local Abelian gauge invariance in the theory. This idea was" @default.
- W2963757816 created "2019-07-30" @default.
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- W2963757816 date "2011-10-17" @default.
- W2963757816 modified "2023-09-24" @default.
- W2963757816 title "Building Gauge Theories: The Natural Way" @default.
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