Why are particles in low representations in the Standard Model?

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Discussion Overview

The discussion revolves around the representation of particles in the Standard Model (SM) of particle physics, specifically why fermions are placed in low representations such as doublets of SU(2) rather than higher representations. Participants explore analogies with other gauge groups, such as SU(5), and consider the implications of different representations on particle properties and quantum numbers.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • One participant questions the rationale for placing fermions in low representations, specifically asking why left-handed electrons and neutrinos are in an SU(2) doublet rather than a triplet.
  • Another participant argues that placing them in a triplet would necessitate the existence of an additional unseen particle, which is not observed.
  • A different viewpoint suggests that higher representations, such as a 6-plet, could accommodate all leptons, but this raises concerns about maintaining correct quantum numbers.
  • One participant proposes that leptons could still be color neutral and share the same isospins and U(1) charges, suggesting that the lepton number symmetry might be an accidental feature of the SM.
  • Another participant counters that a 6-plet representation cannot yield the same isospins for all leptons, citing angular momentum considerations and the requirements of SU(2) representations.
  • A later reply emphasizes that the particle content of the Standard Model is not theoretically derived but rather based on empirical observations, highlighting the model's reliance on free parameters.

Areas of Agreement / Disagreement

Participants express differing views on the appropriateness of higher representations for fermions in the Standard Model, with no consensus reached on the validity of these representations or their implications for particle properties.

Contextual Notes

Participants note limitations in deriving the particle content of the Standard Model theoretically, indicating that the discussion is grounded in empirical input rather than a definitive theoretical framework.

ChrisVer
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I was wondering.
What's the reason for putting objects in low representations in the SM and not higher ones?
So, why fermions in a doublet of SU(2) and not a multiplet?

In analogy in SU(5) we put the particles in the 5-plet...
 
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You could do that. But it would predict particles that are unseen. If I put the left-handed electron and neutrino in an SU(2) triplet and not an SU(2) doublet, where is the third particle?
 
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Hmmm I was thinking more the representations of the same gauge group.
For example the SU(2) has the 4-plet or triplet representation
(
2 \otimes 2 = 3 \oplus 1
2 \otimes 3 = 4 \oplus 2
)

and in a similar way I think you can work up to the 6plet.
In the 6plet one could put all the leptons.
 
You can't do that and make the quantum numbers come out right. How do the e and mu get the same quantum numbers if they are in different positions in the multiplet?
 
I think they would still be color neutral...
They would still have the same isospins and u(1) charges, and that's enough.
For example if I had:
[6] = \begin{pmatrix} e \\ \nu_e \\ \mu \\ \nu_\mu \\ \tau \\ \nu_\tau \end{pmatrix}

The U(1) transformation matrix would have to be Y_6 = \begin{pmatrix} Y_{el-flav} & 0 & 0 \\ 0 & Y_{mu-flav} & 0 \\ 0 & 0 & Y_{tau-flav} \end{pmatrix}
(still traceless) with Y_{i-flav} the same 2x2 matrices you have in the SM for the i-th flavor.
and similarily for the isospin
T_6^i = diag ( \tau^i , \tau^i , tau^i )
The only quantum number which I "feel" this would violate is the lepton number. But the lepton number is an accidental symmetry of SM.

Maybe I'm terribly wrong with the choices of Y and T matrices?
 
You can't have them in a 6-plet of isospin and have the same isospins.

Consider angular momentum, also an SU(2). A 6-plet corresponds to J=5/2 which has m = +/- 5/2, +/- 3/2 and +/- 1/2. You can't declare it to have three +/- 1/2 and no +/- 3/2 or +/- 5/2. That's not a J=5/2 state and it's not a 6-plet.
 
There's no way (yet?) to derive the particle content of the Standard Model theoretically. It's just empirical input to the model. The same holds for the many free parameters (coupling constants/masses).
 

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