Standard model + symmetry questions

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Homework Help Overview

The discussion revolves around the gauge invariances of the Standard Model, specifically U(1), SU(2), and SU(3), and their associated quantum numbers. Participants explore the implications of non-abelian symmetries for interactions between force carriers and the expression for local gauge transformations acting on quark spinors.

Discussion Character

  • Exploratory, Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants discuss the gauge symmetries and their roles in fundamental interactions, questioning the nature of the U(1) symmetry in the weak sector and the implications of non-abelian gauge invariance compared to abelian ones. There are attempts to clarify the expression for SU(3) transformations acting on quark fields.

Discussion Status

Some participants are providing clarifications and corrections regarding the electroweak symmetry and its breaking, while others are attempting to refine their understanding of the gauge transformations and quantum numbers involved. The conversation reflects a mix of interpretations and ongoing exploration of the concepts.

Contextual Notes

There are indications of confusion regarding the specific roles of the U(1) symmetries and the nature of gauge invariance in the context of the Standard Model, particularly in relation to spontaneous symmetry breaking.

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Homework Statement



1) Which U(1), SU(2) and SU(3) gauge invariances are implemented in nature according to the Standard Model? What are the related quantum numbers?

2) The SU(2) symmetry is referred to as a non-abelian symmetry. What does this imply for the interactions between the force carriers?

3) Give the expression for a SU(3) local gauge transformation acting on a quark spinor triplet.

2. The attempt at a solution

1) Gauge symmetries in the SM, used describe three of the fundamental interactions, are based of the SU(3)xSU(2)xU(1) group. Roughly speaking the symmetries of the SU(3) group describe the stronge force, the SU(2) group the weak interaction and U(1) the electromagnetic force.

2) The electroweak model breaks parity maximally. All its fermions are chiral Weyl fermions, which means that the charged weak gauge bosons only couple to left-handed quarks and leptons (making this a non-abelian symmetry).

3) ?
 
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Ad 1) Think again about the SU(2) x U(1) in the weak sector. Is this (!) U(1) really the em. U(1)?

Ad 2) What's the point about non-Abelian gauge invariance compared to an Abelian one? Think about the interactions of the non-Abelian gauge bosons in contrast to that of Abelian ones!

Ad 3) How does the color gauge group act on the quark fields? It's pretty "fundamental" ;-)).
 
Okay, thank you! Another shot, still not perfect though:

1) U(1) -> Photon (QED). Quantum number Q
SU(2) - > W+, W- and Z-boson (electroweak interaction), Quantum number Y
SU(3) -> 8 gluons (QCD) (Gell-Mann Matrices), Quantum number T3

2) The force carriers self-interact so W-W+ \otimes Z

3) ψ = Uψ where ψ is the quark field, a dynamical function of space-time, in the fundamental representation of SU(3) and U the gell-mann matrices.
 
Last edited:
The electroweak part of (1) is not yet correct. Note that SU(2) X U(1) is the symmetry group before "spontaneous symmetry breaking" of the gauge group. It's spontaneously broken to another (1) U(1), which latter is the em. U(1) associated with electric charge! The former U(1) is the group associated with weak hypercharge, Y!
 
Thanks!
 

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