Why must the mediator of the strong force be heavy?

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SUMMARY

The discussion centers on the necessity of a heavy mediator for the strong force, as proposed by Yukawa. A massless mediator would result in a Coulomb potential, indicating a long-range force, while a massive mediator leads to a Yukawa potential, characterized by a negative exponential that suppresses the potential with increasing mass, thus resulting in a shorter range. The strong force is mediated by massless gluons, but due to confinement, only colorless states are observable at lower energies, preventing a Coulomb-like behavior.

PREREQUISITES
  • Understanding of Yukawa potential and its implications
  • Familiarity with the concept of massless and massive mediators
  • Knowledge of gluons and their role in the strong force
  • Basic grasp of confinement in quantum chromodynamics (QCD)
NEXT STEPS
  • Study the Yukawa potential in detail, focusing on its mathematical formulation
  • Explore the concept of confinement in quantum chromodynamics (QCD)
  • Review Griffith's Introduction to Elementary Particles, specifically Problem 1.2
  • Investigate the role of gluons in mediating the strong force and their properties
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Students of particle physics, theoretical physicists, and anyone interested in the fundamental forces of nature and their mediators.

Phys12
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I'm reading Griffith's Introduction to Elementary Particles and it says that when Yukawa proposed his theory of the strong force, it was an indication that the meadiator of that force must be a heavy particle since the force is a short ranged force. Why is that the case? I cannot get the intuition behind it
 
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A massless mediator leads to a Coulomb potential - it has a long range. A massive mediator leads to a Yukawa potential, where larger masses lead to shorter ranges.
 
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Look at the (negative!) exponential in the yukawa potential. It surpresses the potential if the mass of the mediator gets larger.
 
Also note that this is the residual strong force mediated by pions. The strong force itself is mediated by massless gluons. The reason that this does not lead to a Coulomb potential is confinement, i.e., that only colourless states exist at lower energies.
 
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Phys12 said:
Why is that the case?

You know how right after he writes that, Griffiths says "See Problem 1.2"? You should see problem 1.2.
 

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