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Everything about Yukawa Interaction totally explained

In particle physics, Yukawa interaction, named after Hideki Yukawa, is an interaction between a scalar field phi and a Dirac field Psi of the type:V approx garPsi phi Psi (scalar) or g ar Psi gamma^5 phi Psi (pseudoscalar).
   The Yukawa interaction can be used to describe the strong nuclear force between nucleons (which are fermions), mediated by pions (which are pseudoscalar mesons). The Yukawa interaction is also used in the Standard Model to describe the coupling between the Higgs field and massless quark and electron fields. Through spontaneous symmetry breaking, the fermions acquire a mass proportional to the vacuum expectation value of the Higgs field.

The action

The action for a meson field φ interacting with a Dirac fermion field ψ is » S[phi,psi]=int d^dx ;left[

mathcal(m+g phi)^* chi^dagger sigma^2 chi^* ight]

where g is a complex coupling constant and m is a complex number.

Feynman rules

The article Yukawa potential provides a simple example of the Feynman rules and a calculation of a scattering amplitude from a Feynman diagram involving the Yukawa interaction.

Further Information

Get more info on 'Yukawa Interaction'.


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