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How could electrically charged particles be massless before the symmetry breaking? Wouldn't the energy stored in the electric field contribute to particles mass?
Electrically charged particles can be massless before symmetry breaking due to the Higgs mechanism, which is integral to the Standard Model of particle physics. The Higgs field, present throughout space, breaks symmetry laws of the electroweak interaction, resulting in the mass acquisition of gauge bosons at temperatures below a critical threshold. This mechanism also explains the mass of fundamental particles like electrons and quarks. In massless Quantum Electrodynamics (QED), the electric field behaves differently, leading to a logarithmic decrease in electric charge at long distances, which prevents long-range Coulomb forces.
PREREQUISITESPhysicists, students of particle physics, and anyone interested in the fundamental principles of mass and charge in the context of the Standard Model.