Hamiltonian formulation of QCD and nucleon mass

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SUMMARY

The discussion focuses on the Hamiltonian formulation of Quantum Chromodynamics (QCD) in Coulomb gauge, specifically regarding the contributions of individual terms in the Hamiltonian to nucleon mass. Key terms identified include quark-gluon interactions and multi-gluon interactions, which significantly influence nucleon mass through binding energy rather than quark mass. The "Constituent quark and spin-spin interaction" model is recommended for a phenomenological approach to estimating hadron masses. Relevant papers include the original reference from Physical Review D and an explanatory document available on arXiv.

PREREQUISITES
  • Understanding of Quantum Chromodynamics (QCD)
  • Familiarity with Hamiltonian mechanics in quantum field theory
  • Knowledge of non-perturbative methods in particle physics
  • Experience with phenomenological models in hadron mass calculations
NEXT STEPS
  • Read the paper "Constituent quark and spin-spin interaction" for insights on hadron mass estimation
  • Explore the original reference in Physical Review D for foundational concepts
  • Analyze the paper available at arXiv: hep-ph/0412098v2 for detailed explanations
  • Investigate the analysis presented in arXiv: 1310.1797v1 for further understanding of nucleon mass
USEFUL FOR

Researchers in theoretical physics, particularly those specializing in particle physics, quantum field theory, and anyone studying the mass dynamics of nucleons and hadrons.

tom.stoer
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Hello,

there are several papers on QCD in Hamiltonian formulation, especially in Coulomb gauge. Unfortunately the Hamiltonian H is rather formel and highly complex.

Question: is there a paper discussing the contribution of individual terms of H to the nucleon mass?
 
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The question about nucleon masses is rather complicated by itself, especially because it is a non-perturbative problem. I don't know if there is any simple way to related any term in the QCD Hamiltonian to the nucleon mass. I would say that the most relevant terms are the quark-gluon interaction and the gluon-gluon-gluon or gluon-gluon-gluon-gluon interactions. This is because the nucleon (or in general hadron) masses are mainly given by binding energy rather then the actual quark masses.

However, if you want a more phenomenological way of deriving (with a pretty good accuracy) the mass of the hadrons you can take a look at the "Constituent quark and spin-spin interaction" model. I think that the original reference should be:

http://journals.aps.org/prd/abstract/10.1103/PhysRevD.12.147

However, there is a pretty good explanation of that in:

http://arxiv.org/pdf/hep-ph/0412098v2.pdf

In section II.

I hope this is useful.
 
Einj said:
The question about nucleon masses is rather complicated by itself, especially because it is a non-perturbative problem. I don't know if there is any simple way to related any term in the QCD Hamiltonian to the nucleon mass. I would say that the most relevant terms are the quark-gluon interaction and the gluon-gluon-gluon or gluon-gluon-gluon-gluon interactions. This is because the nucleon (or in general hadron) masses are mainly given by binding energy rather then the actual quark masses.
Yes, I know.

What I am looking for us an analysis like

http://arxiv-web3.library.cornell.edu/pdf/1310.1797v1.pdf

for the nucleon mass.
 

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