Why Do Electron, Muon, and Tau Masses Differ in Scale and Correction Effects?

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SUMMARY

The discussion centers on the differences in mass scales and loop corrections for electrons, muons, and taus within the Standard Model of particle physics. It is established that these masses differ due to their inherent values, which arise from Yukawa interactions, and the loop corrections that modify these values. The conversation also touches on the possibility of relationships between lepton masses, referencing the Koide formula, and emphasizes the importance of calculating one-loop corrections to the two-point function for fermions. Key texts, such as the quantum field theory book by Schwarz, are recommended for further understanding.

PREREQUISITES
  • Understanding of Standard Model particle physics
  • Familiarity with Yukawa interactions
  • Knowledge of quantum field theory (QFT) concepts
  • Ability to calculate two-point functions for fermions
NEXT STEPS
  • Study the calculation of one-loop corrections in quantum field theory
  • Research the Koide formula and its implications for lepton masses
  • Explore the concept of renormalization in fixed order perturbation theory
  • Read Schwarz's quantum field theory book for detailed explanations of loop diagrams
USEFUL FOR

Physicists, particularly those specializing in particle physics and quantum field theory, as well as students seeking to deepen their understanding of lepton mass scales and loop corrections.

DuckAmuck
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This is a 3 part question.

1. I've come to understand that the mass values in the mass terms (pole mass) of the standard model don't represent what we actually measure. That there are loop corrections. (I understand the concept: there's screening either adding or subtracting from the true value). I get that this is also related to energy scale.
So now, my question is, why is it said that electrons, muons and tau masses are on different scales? Is it just because their masses are so different, or are their loop corrections different, or is it both?

2. Even though the lepton masses are on different scales, is it possible to have a relationship or some kind between them, sort of like the koide formula? Are the pole-masses on the same footing? Could something like the Koide formula have physical meaning?

3. How exactly are loop corrections added? All I know is how to solve for equations of motion from a lagrangian. Where do the loop corrections actually come in? Is there an easy-to-follow walk thru for this?

thank you
 
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Hello,

I would believe this statement of the scales refers just to the fact that they have different masses (which are orders of magnitudes apart).

In the SM, these are just numbers (as a result of yukawa interactions whose strength must be measured experimentally).

Do you know how to calculate a two point function for a fermion? I.e. I( Slashed(p) - m )

The inverse of this gives you the propagatir for a fermion, and the position of the pole gives you the pole mass. At leading order all mass definitions are equivalent/redundant.

Then, the next step is to calculate the one loop correction to the two point function. so all possible 1particle irreducible diagrams. (This is covered in all decent qft books).

The problem is then that these loop diagrams contain divergences. These are subtracted out, and in addition sometimes finite parts. Depending on what is subtracted gives you a different scheme.

The pole scheme corresponds to subtracting the divergent pieces and a residual scale dependence (a result of performing renormalisation in fixed order perturbation theory).

Some texts which discuss this well are the qft book of schwarz
 

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