In physics, a gauge theory is a type of field theory in which the Lagrangian does not change under local transformations according to certain smooth families of operations .
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In physics, a gauge theory is a type of field theory in which the Lagrangian does not change under local transformations according to certain smooth families of operations .
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Gauge theory fields are included in the Lagrangian to ensure its invariance under the local group transformations .
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When such a theory is quantized, the quanta of the gauge fields are called gauge bosons.
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Gauge theory theories are important as the successful field theories explaining the dynamics of elementary particles.
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Gauge theory theories became even more attractive when it was realized that non-abelian gauge theories reproduced a feature called asymptotic freedom.
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In other words, the distinguishing characteristic of a gauge theory is that the gauge field does not merely compensate for a poor choice of coordinate system; there is generally no gauge transformation that makes the gauge field vanish.
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Gauge theory theories used to model the results of physical experiments engage in:.
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The starting point of a quantum field theory is much like that of its continuum analog: a gauge-covariant action integral that characterizes "allowable" physical situations according to the principle of least action.
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Gauge theory field is an element of the Lie algebra, and can therefore be expanded as.
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The interpretation of the interaction Lagrangian in quantum field theory is of scalar bosons interacting by the exchange of these gauge bosons.
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Gauge theory theories are usually discussed in the language of differential geometry.
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Some symmetries of the classical Gauge theory are then seen not to hold in the quantum Gauge theory; a phenomenon called an anomaly.
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