Charged particles mass before symmetry breaking

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SUMMARY

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.

PREREQUISITES
  • Understanding of the Standard Model of particle physics
  • Familiarity with the Higgs mechanism
  • Knowledge of Quantum Electrodynamics (QED)
  • Basic concepts of symmetry breaking in physics
NEXT STEPS
  • Research the Higgs boson and its role in mass acquisition
  • Explore the implications of the Higgs field on gauge bosons
  • Study the effects of symmetry breaking on particle interactions
  • Investigate the properties of massless particles in Quantum Electrodynamics
USEFUL FOR

Physicists, students of particle physics, and anyone interested in the fundamental principles of mass and charge in the context of the Standard Model.

Geanta
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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?
 
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I didn't know there were any electrically charged massless particles.
It is interesting to contemplate an electric charge moving through space at light speed.
I guess it would be able to gain or loose energy on the fly.
 
Is the following relevant to the OP question?

From https://en.wikipedia.org/wiki/Higgs_boson#Higgs_field
According to the Standard Model, a field of the necessary kind (the Higgs field) exists throughout space and breaks certain symmetry laws of the electroweak interaction. Via the Higgs mechanism, this field causes the gauge bosons of the weak force to be massive at all temperatures below an extreme high value. When the weak force bosons acquire mass, this affects their range, which becomes very small. Furthermore, it was later realized that the same field would also explain, in a different way, why other fundamental constituents of matter (including electrons and quarks) have mass.​
 
The electric field for massless QED is very different from what you're used to. Specifically, the electric charge will go to zero logarithmically at long distances, so you won't have long-range Coulomb forces. The heuristic behind this is that it becomes "cheap" to create virtual massless particle-antiparticle pairs which screen any charge. Then it takes arbitrarily little energy to add another particle-antiparticle pair.
 
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