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Ranku
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Would it be correct to represent the energy of massless particles before electroweak symmetry breaking as ##E = cp##, just as we do with photons post-symmetry breaking?
Ranku said:Would it be correct to represent the energy of massless particles before electroweak symmetry breaking as ##E = cp##, just as we do with photons post-symmetry breaking?
Gaussian97 said:this equation is a kinematic equation, therefore it should not care about the dynamic process that gives mass to the particles
Gaussian97 said:even after SSB, if a particle acquires a mass ##m_0## is still not correct to write ##E=\sqrt{p^2+m_0^2}##, but rather you need the renormalized mass
Massless particles are particles that have no rest mass, meaning they have no physical weight or mass at rest. They only have energy and momentum.
Electroweak symmetry breaking is a phenomenon that occurs in particle physics where the electroweak force, which unifies the electromagnetic and weak nuclear forces, breaks into two separate forces at high energies.
Before electroweak symmetry breaking, all particles are massless and have no physical weight. However, after the breaking, some particles acquire mass through interactions with the Higgs field, while others remain massless.
The energy of massless particles before electroweak symmetry breaking is equivalent to their momentum, as they have no rest mass. This energy is constantly changing and can be affected by interactions with other particles or fields.
After electroweak symmetry breaking, some particles acquire mass and therefore have a fixed energy, while others remain massless and continue to have energy equivalent to their momentum. However, the interactions between particles and fields can still affect the energy of all particles, including massless ones.