SUMMARY
The strong nuclear force, responsible for binding protons within an atomic nucleus, weakens with increasing distance due to the negative beta function of SU(3) in quantum field theory. As the nucleus expands, the gauge self-interaction terms dominate over quark content, causing the strong interaction coupling constant to increase. This results in color confinement, where it becomes energetically favorable to create new particles rather than separate colored charges. The residual strong force, mediated by massive pions, leads to interactions resembling Yukawa potentials, with an exponentially suppressed range determined by the pion mass.
PREREQUISITES
- Introductory understanding of quantum field theory
- Familiarity with SU(3) gauge theory
- Basic knowledge of particle physics, including baryons and mesons
- Understanding of Yukawa potentials and their implications
NEXT STEPS
- Study the implications of the beta function in SU(3) gauge theory
- Explore the concept of color confinement in quantum chromodynamics (QCD)
- Learn about the role of pions in mediating residual strong interactions
- Investigate the Yukawa potential and its applications in particle physics
USEFUL FOR
Graduate students in physics, particle physicists, and researchers interested in the fundamental forces of nature and quantum field theory.