In particle physics, what does 'coupling' mean?

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SUMMARY

In particle physics, 'coupling' refers to the interaction between particles, such as how the Higgs boson couples to light particles or how photons couple to charged particles. The coupling constant, often dimensionless, quantifies the strength of these interactions, with values greater than 1 indicating strong coupling and values less than 1 indicating weak coupling. Weak couplings allow the use of perturbation theory, while strong couplings require alternative problem-solving methods. Dimensionful couplings depend on specific energy scales, such as the Planck scale, to determine their strength.

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  • Understanding of particle interactions and fundamental forces
  • Familiarity with coupling constants in quantum field theory
  • Knowledge of perturbation theory in physics
  • Basic concepts of energy scales in particle physics
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  • Investigate the significance of the Planck scale in gravitational interactions
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Particle physicists, theoretical physicists, and students studying quantum field theory will benefit from this discussion on coupling and its implications in particle interactions.

ryanwilk
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Hi,

In particle physics, what does 'coupling' mean? I can't find a definition anywhere and books just assume you know what it is. For example, "the Higgs couples to light particles".

Also, what does it mean to say that something strongly or weakly couples to something else?

Any help would be appreciated.
Thanks.
 
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"coupling" is really just fancy-talk for "interaction". For example when you say "the photon couples to charge", you mean "the photon interacts with particles that have charge." A "coupling constant" is a parameter of the theory (usually dimensionless but not always) that determines the strength of the interaction. Often in practice, we drop the word "constant" since by the context it is always clear what you mean.

If the coupling constant is dimensionless, you can talk about "strong" or "weak" by whether or not the coupling is greater than or less than 1 (sometimes you also have factors of \pi in the formulas, but let's not worry too much about that!). If the coupling is "weak" (< 1) then you can apply the technique of "perturbation theory". Therefore we often use the word "perturbative" to mean "weak".

At "strong coupling" (> 1) you cannot use perturbation theory and you must try to solve the problem some other way. This is the challenge! This is what happens in the strong nuclear force at low energies, for example.

For dimensionful couplings, you can only talk about "strong" or "weak" WITH RESPECT TO SOME SCALE, where "scale" means some fixed energy. So for example, the Newton constant has dimensions of 1/energy^2 (when \hbar=c=1). So that means that the gravity is "weak" when the energy of the particles is smaller than G_N^{-1/2}, and "strong" when it is greater. This energy scale is the "Planck scale" at roughly 10^{18} GeV, far higher energies than anything we can produce in accelerators. So this is why particle physicists say that "gravity is weakly coupled."
 
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