Standard model + symmetry questions

In summary, the Standard Model implements U(1), SU(2), and SU(3) gauge invariances to describe three fundamental interactions. The related quantum numbers are Q for the photon (QED), Y for the W+, W-, and Z-bosons (electroweak interaction), and T3 for the 8 gluons (QCD). The SU(2) symmetry is non-abelian, meaning the force carriers self-interact. A SU(3) local gauge transformation on a quark spinor triplet is represented by ψ = Uψ, where ψ is the quark field and U is the Gell-Mann matrices. The electroweak part of the gauge group is
  • #1
aoner
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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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  • #2
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" ;-)).
 
  • #3
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+ [itex]\otimes[/itex] 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.
 
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  • #4
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!
 
  • #5
Thanks!
 

FAQ: Standard model + symmetry questions

1. What is the Standard Model?

The Standard Model is a theory in particle physics that describes the fundamental particles and their interactions through the strong, weak, and electromagnetic forces. It is currently the most widely accepted theory for understanding the building blocks of matter and their behavior.

2. What is symmetry in the context of the Standard Model?

Symmetry in the Standard Model refers to the concept that the laws of physics are the same for all observers, regardless of their location or orientation in space. This symmetry is important in understanding the behavior of particles and their interactions.

3. How does the Higgs mechanism relate to symmetry in the Standard Model?

The Higgs mechanism is a fundamental part of the Standard Model that explains how particles acquire mass. It is also connected to the concept of symmetry breaking, where the symmetries of the equations describing the particles are broken at high energies, resulting in the particles having different masses at lower energies.

4. What is the role of symmetry in the search for new physics beyond the Standard Model?

Symmetry plays a crucial role in the search for new physics beyond the Standard Model. Many theories propose new symmetries that could help explain unanswered questions, such as the hierarchy problem or dark matter. By testing for new symmetries, scientists hope to uncover new physics and expand our understanding of the universe.

5. What are the current challenges and limitations of the Standard Model and its symmetries?

While the Standard Model has been incredibly successful in predicting and explaining many phenomena, it still has limitations and challenges. For example, it does not include gravity or account for dark matter. Additionally, the symmetries of the model are not yet fully understood and may require further refinement or modification in the future.

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