Renormalization of Bound States in QFT

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SUMMARY

The discussion focuses on the renormalization of bound states in Quantum Field Theory (QFT), specifically referencing Chapter 10 of Itzykson and Zuber's "Quantum Field Theory" as a foundational resource. Effective field theories such as Non-Relativistic Quantum Electrodynamics (NRQED) and Non-Relativistic Quantum Chromodynamics (NRQCD) are essential for understanding bound states, particularly in the context of the Lamb shift in hydrogen. The conversation highlights the importance of summing ladder Coulomb exchanges to accurately describe bound states and suggests further reading on potential NRQED for detailed calculations.

PREREQUISITES
  • Quantum Field Theory (QFT) fundamentals
  • Itzykson and Zuber's "Quantum Field Theory" Chapter 10
  • Non-Relativistic Quantum Electrodynamics (NRQED)
  • Effective field theories in particle physics
NEXT STEPS
  • Study the Lamb shift calculations in NRQED
  • Research potential NRQED and its applications
  • Explore Non-Relativistic Quantum Chromodynamics (NRQCD) for heavy quark bound states
  • Investigate Heavy Quark Effective Theory (HQET) and chiral perturbation theory for light quarks
USEFUL FOR

Physicists, researchers in Quantum Field Theory, and students studying particle physics, particularly those interested in the renormalization of bound states and effective field theories.

Orion Pax
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Hi, I am about to work on the problem of trying to find a renormalization program for bound states in QFT. Any suggestions/advice on where to start would be much appreciated.
 
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You could start with Chapter 10 of Itzykson and Zuber's Quantum Field Theory, which discusses renormalization for bound states, and then look at some of the papers they refer to.
 
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john baez said:
You could start with Chapter 10 of Itzykson and Zuber's Quantum Field Theory, which discusses renormalization for bound states, and then look at some of the papers they refer to.
Thanks, I'm on it!
 
When we are calculating the loop corrections in our theory (QED, for instance), how does the fact that our electron is in a bound state show itself in the renormalization? Does it matter at all? If so, then why are the predicted values for the Lamb shift, which are calculated in QFT for the electron in Hydrogen, i.e for a bound state, in such close agreement with experiment? Am I missing something here? Thanks
 
Orion Pax said:
When we are calculating the loop corrections in our theory (QED, for instance), how does the fact that our electron is in a bound state show itself in the renormalization? Does it matter at all? If so, then why are the predicted values for the Lamb shift, which are calculated in QFT for the electron in Hydrogen, i.e for a bound state, in such close agreement with experiment? Am I missing something here? Thanks
The modern approach to QFT in bound states is through the use of effective field theories. For QED bound states, look for NRQED (non relativistic QED). Look for a paper on Lamb shift in NRQED to see the details. The renormalization is done as usual in an effective field theory, the bound state part shows up only in the fact that the asymptotic state is not free particles but a bound state, effectively one must sum up all the ladder Coulomb exchanges to infinity and this corresponds to the asymptotic state being a bound state satisfying Schrödinger's equation with a Coulomb potential. Again, see my paper on Lamb shift in NRQED for details on the Lamb shift calculation in this approach (look also for papers on "potential NRQED").

If your ultimate goal is to study quark bound states, an effective field theory approach is also required. For bound states of heavy quarks, look for NRQCD and potential NRQCD. For bound state of one heavy quark plus light quarks, look for HQET. For light quarks only, one need chiral perturbation theory.
 

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