Abstract
We want to study the typical behavior of physical fields near a ground state (also called vacuum). It happens frequently that the ground state of a many-particle system is not unique. In this case, the system can oscillate near different ground states which, as a rule, corresponds to different physical behavior. Therefore, the choice of the ground state plays a crucial role. Historically, Pauli criticized the formulation of gauge field theories by Yang and Mills in 1954; Pauli emphasized that the corresponding interacting gauge particles are massless, in contrast to physical experiments. This defect of gauge theories could be cured in the 1960s by using the so-called Higgs mechanism which equips the gauge bosons with mass. This way, the W ±-bosons and the Z 0-boson obtain their mass in the Standard Model of particle physics. Physicists speak of symmetry breaking (or loss of symmetry) for the following reason.
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The original theory possesses a family of ground states which can be transformed into each other by using the symmetry group \(\mathcal{G}\) of the theory.
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In nature, physical systems oscillate frequently near a distinguished ground state. These realistic states are not anymore symmetric under the original symmetry group \(\mathcal{G}\). In this sense, the symmetry group \(\mathcal{G}\) is broken.
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© 2011 Springer-Verlag Berlin Heidelberg
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Zeidler, E. (2011). Symmetry Breaking. In: Quantum Field Theory III: Gauge Theory. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-642-22421-8_15
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DOI: https://doi.org/10.1007/978-3-642-22421-8_15
Publisher Name: Springer, Berlin, Heidelberg
Print ISBN: 978-3-642-22420-1
Online ISBN: 978-3-642-22421-8
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