Physical interpretation of V and A couplings

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SUMMARY

The discussion centers on the physical differences between vector (V) and axial (A) couplings in quantum field theory, specifically in the context of chiral fermions. The vector coupling is represented as \(\bar{\psi}\gamma^\mu\psi\), while the axial coupling is expressed as \(\bar{\psi}\gamma^\mu\gamma^5\psi\). The conversation highlights that mixed terms, such as \(\bar{\psi}\gamma^\mu(1-\gamma^5)\psi\), can lead to parity violation, particularly in processes like beta decay where the V-A interaction results in negative helicity for outgoing leptons. The mathematical demonstration of parity violation through the eigenvalue properties of the parity operator is also discussed.

PREREQUISITES
  • Understanding of quantum field theory concepts, particularly vector and axial currents.
  • Familiarity with Dirac matrices, specifically \(\gamma^\mu\) and \(\gamma^5\).
  • Knowledge of chiral fermions and their representations in Lagrangians.
  • Basic principles of parity violation in particle physics.
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  • Study the mathematical properties of Dirac matrices, focusing on \(\gamma^5\) and its implications in quantum field theory.
  • Research the role of V-A interactions in weak decays, particularly in beta decay processes.
  • Examine the implications of parity violation in various particle interactions and how it affects conservation laws.
  • Explore advanced topics in quantum field theory, such as the implications of mixed terms in Lagrangians and their physical interpretations.
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Particle physicists, quantum field theorists, and students studying the intricacies of weak interactions and parity violation in particle physics.

bomanfishwow
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Hi,

I'm trying to remind myself of exactly what, physically, is the difference between V and A couplings. Now, a vector coupling is of the form \bar{\psi}\gamma^\mu\psi, and axial coupling of the form \bar{\psi}\gamma^\mu\gamma^5\psi. Thinking in terms of a chiral fermion expanded as:

<br /> f = \left[\left(\frac{1-\gamma^5}{2}\right) + \left(\frac{1+\gamma^5}{2}\right)\right]\psi<br />

and where \bar{f} = \gamma^\dagger\gamma^0, I assume the difference between the V and A couplings has to do with how the L and R projection operators commute through either \gamma^\mu or \gamma^\mu\gamma^5 from the 'coupling' term, and the \gamma^0 from the conjugate field term in a given Lagrangian.

However, as [\gamma^5,\gamma^5] = 0, I don't see how a difference in the chiral treatment between V and A couplings can arise. Am I barking up completely the wrong tree? Any insight welcomed!
 
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You can always redefine what you mean by "V" and "A", as purely vector or purely axial currents conserve parity. It's the mixed terms that generate parity violation.
 
Vanadium 50 said:
You can always redefine what you mean by "V" and "A", as purely vector or purely axial currents conserve parity. It's the mixed terms that generate parity violation.

So, a mixed term is something like \bar{\psi}\gamma^\mu\left(1-\gamma^5\right)\psi? How can it be shown that this term violates parity?

Cheers.
 
Gamma 5 is a pseudoscalar. Adding a pseudoscalar to a scalar violates parity.
When used in beta decay, the V-A interaction leads to negative helicity for outgoing leptons. This violates parity.
 
clem said:
Gamma 5 is a pseudoscalar. Adding a pseudoscalar to a scalar violates parity.

Sure, but I'm interested in showing why this is the case mathematically...
 
Given P|\psi&gt; = (-1)^n|\psi&gt;

Then P(a + b\gamma^5)|\psi&gt; = aP|\psi&gt; + bP \gamma^5|\psi&gt;

Which is \left( (-1)^na + (-1)^{n+1}b \right) |\psi&gt;, so is only an eigenvalue of parity if a=0 or b=0.
 
Ah yes, very elegant. Thanks!
 

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