Understanding Electron Chirality and Scalar Conservation

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Discussion Overview

The discussion revolves around the chirality of electrons and positrons, specifically addressing the claims about their chiral properties and the implications of scalar couplings in particle physics. Participants explore theoretical aspects, terminology, and references to literature, including Flip Tanedo's article on the subject.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • Some participants assert that electrons are left chiral and positrons are right chiral, while others challenge this by stating that a positron and an anti-electron are the same entity, leading to contradictions in the claims.
  • There is a discussion about the terminology used to describe the components of Dirac spinors, with some participants suggesting that the terms "electron" and "anti-electron" are misapplied.
  • One participant explains that the chirality of spinor components depends on the basis chosen (Weyl vs. Dirac), indicating that chirality is not fixed and can vary based on the representation used.
  • Participants mention the mass term coupling left and right chirality and the kinetic term coupling terms of the same chirality, highlighting the complexity of the relationships between these concepts.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the chirality of electrons and positrons, with multiple competing views presented. The discussion remains unresolved regarding the correct interpretation of chirality in the context of the referenced literature.

Contextual Notes

There are limitations in the discussion regarding the definitions of terms and the assumptions made about chirality and particle identities. Some participants express confusion stemming from the terminology used in the literature, which may contribute to differing interpretations.

kimcj
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(1) electron = left chiral . anti electron = right chiral. positron = left chiral. anti positron = right chiral. So scalar couples L and R chiral fermion fields.
(2)electron = left chiral . anti electron = right chiral. positron = right chiral. anti positron = left chiral. So scalar conserves chirality.Im pretty sure 1 is right. However in flip tanedos article he says that the anti positron has left chirality...

Is 1 right??

Im definite that (1) is right. However in flip tanedos 'feynman diagrams for undergrads- helicity chirality and the mass' has some confusing phrases saying that the anti positron is left chiral...

Is (1) right??
 
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kimcj said:
in flip tanedos article

Do you have a link to this article?
 
kimcj said:
Is (1) right??

A positron and an anti-electron are the same thing. So are an anti-positron and an electron. So (1) doesn't even make sense; it contradicts itself.
 
PeterDonis said:
A positron and an anti-electron are the same thing. So are an anti-positron and an electron. So (1) doesn't even make sense; it contradicts itself.
No i don't mean the physical mass based electrons and positrons. i mean the spinor componets of the electron and positron
 
kimcj said:
i don't mean the physical mass based electrons and positrons. i mean the spinor componets of the electron and positron

In other words, you are referring to a 4-component Dirac spinor, and you are calling the upper two components the "electron" and "anti-electron", and the lower two components the "positron" and "anti-positron"? That's not correct terminology, and that may be why you are getting apparently different answers from the article you read (do you have a link?).

If you want to view a 4-component Dirac spinor as being "made of" two 2-component Weyl spinors, then the first 2-component spinor would be the "electron" and the second 2-component spinor would be the "positron". It is still true, as I said, that "positron" and "anti-electron" are the same thing, and "anti-positron" and "electron" are the same thing.

The chirality of the components themselves depends on which basis you choose. In the Weyl basis, each 2-component Weyl spinor has definite chirality for both components--the first component is left and the second is right. In the Dirac basis, however, that is not the case. In the Weyl basis, the first 2-component spinor would have components called "left-handed electron" and "right-handed electron", and the second would have components called "left-handed positron" and "right-handed positron".

As far as making scalars out of these spinors, the mass term ##\bar{\psi} m \psi## couples terms of left and right chirality, and the kinetic term ##\bar{\psi} \gamma^{\mu} \partial_{\mu} \psi## couples terms of the same chirality (left and right separately).
 
Just to clarify this, an electron is of course not the same as a positron. The electron is negatively and the positron is positively charged. They are particle and antiparticle, described by massive Dirac (bispinor) field. They are thus not of definite chirality but consist of both left- and right-handed spinor components, as already is clear from the mass term ##\bar{\psi} \psi=\bar{\psi}_L \psi_R + \bar{\psi}_R \psi_L##.

For details, have a look at the first theory lecture here:

http://fias.uni-frankfurt.de/~hees/hqm-lectweek14/index.html
 
PeterDonis said:
By the "Flip Tanedo" article, do you mean this?
yes...
 

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