Weak force and axial vector coupling

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SUMMARY

The discussion centers on the concept of pure axial vector coupling in the context of weak force interactions, specifically regarding the decay of the pi-meson as described in David Griffith's "Introduction to Elementary Particles." The weak force vertex is characterized by the factor γu(1-γ5), where only the term involving γ5 contributes to the interaction. This indicates that certain particle types, particularly quarks in a bound pseudoscalar state, engage in pure axial coupling, while vector contributions are absent due to the nature of their wavefunctions.

PREREQUISITES
  • Understanding of weak force interactions and weak currents
  • Familiarity with the concepts of axial vector and vector currents
  • Knowledge of particle physics terminology, specifically regarding pi-mesons and quarks
  • Basic grasp of gamma matrices and their role in quantum field theory
NEXT STEPS
  • Study the properties of weak currents in particle physics
  • Explore the mathematical framework of axial vector coupling in quantum field theory
  • Investigate the role of gamma matrices in weak interactions
  • Learn about the implications of pseudoscalar states in particle decay processes
USEFUL FOR

Students and researchers in particle physics, particularly those interested in weak interactions, axial vector coupling, and the behavior of mesons and quarks in decay processes.

a dull boy
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Hi physics forum,

I have been reading David Griffith's book "intro to elementary particles" and he
describes the decay of the pi-meson as "pure axial vector"

Can someone tell me what this means, in terms of the weak force vertex consisting of
this factor

γu(1-γ5)

Thanks, Mark
 
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Only the term with the gamma_5 in it contributes.
 
Thanks for the reply. I'll follow up 1) what does that mean physically, for example, do only certain particle types engage in pure axial coupling? 2) can you say a little as how
the math would work (how can the vector part of V-A not contribute, since the axial
part is multiplied by the vector (γuγ5

I am a novice in this, so it may not be a good question! -Mark
 
db, The weak interaction is an interaction between weak currents, JμJμ. For the lepton pair the particles are free, and Jμ is of the V-A form.

However the quarks that make up the pion are not free, they are in a bound pseudoscalar state. You can combine their wavefunction with the 4-momentum kμ to construct an axial vector current, but there is no way to make a vector current.
 
Time reversal invariant Hamiltonians must satisfy ##[H,\Theta]=0## where ##\Theta## is time reversal operator. However, in some texts (for example see Many-body Quantum Theory in Condensed Matter Physics an introduction, HENRIK BRUUS and KARSTEN FLENSBERG, Corrected version: 14 January 2016, section 7.1.4) the time reversal invariant condition is introduced as ##H=H^*##. How these two conditions are identical?

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