EFT & change or coupling constants

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SUMMARY

The discussion focuses on the use of Effective Field Theory (EFT) to analyze interactions at various energy levels while neglecting higher energy interactions. It emphasizes the necessity of changing coupling constants due to their running behavior observed in electromagnetic, weak, and strong force interactions at high energies. Key evidence supporting the absence of additional particles in the Standard Model includes the democratic decay of W and Z bosons, particle-antiparticle creation from high-energy photons, and the successful fitting of collider data with the existing particle set. The running of coupling constants is essential for maintaining consistent observable physics across different renormalization scales.

PREREQUISITES
  • Understanding of Effective Field Theory (EFT)
  • Familiarity with coupling constants and their running behavior
  • Knowledge of the Standard Model of particle physics
  • Basic concepts of particle decay and collider data analysis
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  • Study the implications of the running of coupling constants in Quantum Field Theory
  • Explore the evidence for the Standard Model's particle set through collider experiments
  • Investigate the role of the CKM matrix in particle interactions
  • Learn about the implications of Occam's Razor in theoretical physics
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Particle physicists, theoretical physicists, and researchers interested in the foundations of the Standard Model and the implications of Effective Field Theory in high-energy physics.

StarsRuler
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I understand that by uncertainty relations, it is possible use an EFT to a range of energy, forgotten the interactions for bigger energies. But, ¿ why change the values of coupling costants?

And, ¿ how can tell that there is no intermediate particle that happens with low probability in scatterings that don´t let found the effective lagrangian? ¿ How we can that no more particles in standard model?
 
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The running of the coupling constants is necessary because this is what you observe when you look at EM, weak force and strong force interactions at high energies. The fact that it flows naturally from the procedures you to renormalize and hence to make it possible to do calculations is just an added bonus.

The strongest evidence to date that there are no more particles in the Standard Model are:
(1) W and Z boson decay are "democratic" which is to say that they produce all mass-energy conservation permitted particles in equal amounts (subject to some well understood tweaks). So, weakly interacting particles lighter than the W or Z boson are forbidden. Also, if there was a weakly interacting particle with mass lighter than half the Higgs boson mass and more than half the Z boson mass, the Higgs decays would also be much different than those observed.
(2) Particle-antiparticle creation from high energy photons provides similar assurance with regard to charged particles.
(3) We are able to fit all of the collider data with the particle set of the Standard Model (of course, fitting astronomy observations such as dark matter and inflation and gravity is another matter entirely).
(4) The experimentally observed unitarity of the CKM matrix leaves very little room for additional particles along the lines of SM4.
(5) With a Higgs boson of the mass observed, the equations of the SM don't break down anywhere up to GUT scale energies (as the would at some other Higgs boson masses). So, we don't need a new particle, for example, to keep the probabilities unitary up to an arbitrarily high level.

The SM exclusion of right handed neutrinos and other particles is simply Occam's Razor at work. The SM doesn't need them to explain what is seen so a minimal particle set and force set is assumed until we learn otherwise. For several decades, we needed to Higgs boson for the SM to work even though we didn't see it, so it was inferred. But, no data requires more than three generations of fermions, and no data requires more than the known bosons to explain anything but gravity/astronomy.
 
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The coupling constants "run" because they incorporate the physics of those "forgotten" interactions that you integrate out. The running of the coupling constants is necessary to ensure that the observable physics does not depend on the renormalization scale.
 

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