Physical interpretation of V and A couplings

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Discussion Overview

The discussion centers on the physical interpretation of vector (V) and axial (A) couplings in the context of particle physics, particularly focusing on their mathematical representations and implications for parity violation. Participants explore the differences between these couplings, their definitions, and their effects in processes like beta decay.

Discussion Character

  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant describes the mathematical forms of V and A couplings and questions how their chiral treatment leads to differences in physical interpretation.
  • Another participant suggests that the definitions of V and A can be redefined, noting that purely vector or axial currents conserve parity, while mixed terms lead to parity violation.
  • A participant provides an example of a mixed term and asks for a mathematical demonstration of how it violates parity.
  • It is noted that gamma 5 is a pseudoscalar, and the addition of a pseudoscalar to a scalar is said to violate parity, particularly in the context of beta decay where the V-A interaction results in negative helicity for outgoing leptons.
  • One participant expresses interest in a mathematical proof of the parity violation associated with mixed terms.
  • A mathematical approach is presented that shows how the parity operator acts on a combination of scalar and pseudoscalar terms, indicating conditions under which the combination can be an eigenvalue of parity.

Areas of Agreement / Disagreement

Participants express differing views on the implications of V and A couplings, particularly regarding their definitions and effects on parity. There is no consensus on a definitive explanation or mathematical proof of the parity violation associated with mixed terms.

Contextual Notes

The discussion includes assumptions about the properties of gamma matrices and the nature of parity, which may not be universally accepted or fully resolved within the conversation.

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 [tex]\bar{\psi}\gamma^\mu\psi[/tex], and axial coupling of the form [tex]\bar{\psi}\gamma^\mu\gamma^5\psi[/tex]. Thinking in terms of a chiral fermion expanded as:

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

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

However, as [tex][\gamma^5,\gamma^5] = 0[/tex], 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 [tex]\bar{\psi}\gamma^\mu\left(1-\gamma^5\right)\psi[/tex]? 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 [itex]P|\psi> = (-1)^n|\psi>[/itex]

Then [itex]P(a + b\gamma^5)|\psi> = aP|\psi> + bP \gamma^5|\psi>[/itex]

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

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