What Are the Key Differences Between Fermion and Scalar Field Interactions?

Click For Summary

Discussion Overview

The discussion centers on the differences between fermion and scalar field interactions, specifically examining the implications of coupling a fermion field to a scalar field through different types of interactions. The scope includes theoretical considerations of particle physics and the properties of interactions under various symmetries.

Discussion Character

  • Technical explanation
  • Debate/contested

Main Points Raised

  • Some participants note that the first interaction Lagrangian represents a scalar coupling, while the second represents a pseudoscalar coupling, suggesting a difference in their transformation properties under parity.
  • One participant questions the physical differences between the interactions beyond their transformation properties, indicating a desire for deeper understanding.
  • Another participant emphasizes that the symmetries of the interactions define their modeling capabilities, hinting at a broader context for their applications.
  • A later reply elaborates on the weak force, stating that it preferentially couples to left-handed particles and right-handed anti-particles, and that at tree level, there is no weak coupling to right-handed fields.
  • It is mentioned that the weak coupling can be expressed as a combination of vector and axial vector couplings, with a specific focus on the pure V+A nature of the weak interaction, which exclusively couples to left-handed fields.
  • One participant references an experimental observable, the polarized e+/e- beam experiment of SLD, to illustrate the effects of these couplings.

Areas of Agreement / Disagreement

Participants express varying levels of understanding regarding the implications of scalar versus pseudoscalar couplings, and while some points about transformation properties are acknowledged, the discussion remains unresolved regarding the broader physical implications of these differences.

Contextual Notes

There are limitations in the discussion regarding the assumptions made about the interactions and the specific contexts in which they apply, particularly concerning the weak force and its coupling properties.

jdstokes
Messages
520
Reaction score
1
Suppose I couple a fermion field to a scalar field using [itex]\mathrm{i} g \bar{\psi}\psi \varphi[/itex] and [itex]\mathrm{i} g \bar{\psi}\gamma_5\psi\varphi[/itex].

I'm trying to understand what would be the physical difference between these interactions. I know that [itex](1/2)(1\pm \gamma_5)[/itex] approximately projects out the left and right handed components of Dirac fields and that this is related to the fact that the weak interaction couples preferentially to left-handed particles and right-handed anti-particles, but other than that I'm pretty clueless.
 
Last edited:
Physics news on Phys.org
Your first interaction lagrangian is a scalar coupling, while the second is a pseudoscalar coupling. Check how they both transform under parity.
 
What is the physical difference in the interactions apart from their transformation properties?
 
The symmetries of the interaction define what interactions they are used to model.
 
jdstokes said:
Suppose I couple a fermion field to a scalar field using [itex]\mathrm{i} g \bar{\psi}\psi \varphi[/itex] and [itex]\mathrm{i} g \bar{\psi}\gamma_5\psi\varphi[/itex].

I'm trying to understand what would be the physical difference between these interactions. I know that [itex](1/2)(1\pm \gamma_5)[/itex] approximately projects out the left and right handed components of Dirac fields and that this is related to the fact that the weak interaction couples preferentially to left-handed particles and right-handed anti-particles, but other than that I'm pretty clueless.

The weak force not only prefers left-handed; at tree level there is no weak coupling to right-handed fields.

The weak force is slightly more complicated than your model because vector bosons are vectors (duh). You can write the weak coupling as a sum of alpha*Vector + beta*Axial Vector couplings. Up to an internal minus sign (always mix it up), the weak coupling is pure V+A, so it couples solely to left-handed fields. The most obvious physical observable used to demonstrate this is the polarized e+/e- beam experiment of SLD...
 

Similar threads

  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 2 ·
Replies
2
Views
4K
  • · Replies 3 ·
Replies
3
Views
3K
  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 4 ·
Replies
4
Views
2K
  • · Replies 4 ·
Replies
4
Views
3K
  • · Replies 5 ·
Replies
5
Views
6K
  • · Replies 1 ·
Replies
1
Views
2K