Imagining a Higgsless Universe

  • Context: Undergrad 
  • Thread starter Thread starter nikkkom
  • Start date Start date
  • Tags Tags
    Universe
Click For Summary
SUMMARY

This discussion explores the theoretical implications of a Higgsless universe governed by the Standard Model, specifically focusing on the unbroken SU(2) × U(1) symmetry. Key points include the absence of mass for all elementary particles, the differentiation between left- and right-fermions, and the emergence of new forces characterized by SU(2) weak isospin and U(1) weak hypercharge. The conversation also delves into the complexities of hadron formation, isospin interactions, and the potential for new composite particles, such as leptohadrons, due to the altered dynamics in this hypothetical framework.

PREREQUISITES
  • Understanding of the Standard Model of particle physics
  • Familiarity with SU(2) and U(1) gauge symmetries
  • Knowledge of particle mass generation mechanisms, particularly the Higgs mechanism
  • Basic concepts of quantum chromodynamics (QCD) and particle interactions
NEXT STEPS
  • Research the implications of unbroken SU(2) and U(1) on particle interactions
  • Explore the concept of leptohadrons and their formation in theoretical physics
  • Investigate the role of quark condensates in mass generation and symmetry breaking
  • Examine existing models of technicolor and their relevance to Higgsless theories
USEFUL FOR

Theoretical physicists, particle physicists, and students interested in advanced concepts of gauge theories and the implications of symmetry breaking in the Standard Model.

  • #31
Got reminded of this thread from https://www.physicsforums.com/threa...-second-third-generation.890021/#post-5599190

Vanadium 50 said:
Step 1: set the Higgs coupling to the W and Z to zero. The W and Z masses don't go to zero: they go to about 30 MeV because they still get a QCD mass from the quark condensate.

Step 2: Let's set the Higgs couplings to the quarks to zero. This should set all the 0- masses to a 36-fold degenerate zero, because they are all Goldstones. Other mesons will still be massive, as will the baryons, because their mass is governed by LambdaQCD and not the quark current masses. Surely that will set the W and Z masses to zero. And...now they weigh about 100 keV.
What exactly do you mean by step 1? The Higgs will still be an SU(2) doublet and the coupling is fixed by the SU(2) coupling constant because the interaction term originates in the covariant derivative of the kinetic term for the Higgs field. Putting the Higgs coupling to the SU(2) gauge bosons to zero would imply putting the SU(2) coupling constant to zero and the SU(2) part of the theory would then be free and meaningless. If you make the Higgs an SU(2) singlet, clearly it will no longer couple to the SU(2) gauge bosons, but then you have fundamentally changed the field content of your model. On the other hand, if you do that you will no longer have a scalar doublet that you can use to create the Yukawa couplings that you want to turn off in step 2.
 
Physics news on Phys.org
  • #32
The steps are not intended to be viable, consistent and renomalizable theories on their own. They are there to illustrate the consequences in a simple way. Think of it like removing and then reinserting the corilois force in discussing classical mechanics.
 
  • #33
I don't see why it is interesting to discuss a model where a Higgs boson/field does not exist when there is now good evidence that it does.
 
  • #34
rootone said:
I don't see why it is interesting to discuss a model where a Higgs boson/field does not exist when there is now good evidence that it does.

Well, depends of your view of the goals of discussing. Towards publication of a pheno paper, it is sort of absurd. Towards learning or even as advanced undergraduate work, it is valuable.
 
  • #35
rootone said:
I don't see why it is interesting to discuss a model where a Higgs boson/field does not exist when there is now good evidence that it does.

It helps illustrate the role played by the Higgs.
 
  • #36
We also are happy to let our students play with several hypothetical scenarios in order to understand the theory better. I see no reason why we should not do the same ourselves.
 

Similar threads

  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 9 ·
Replies
9
Views
1K
  • · Replies 12 ·
Replies
12
Views
3K
Replies
7
Views
2K
  • · Replies 6 ·
Replies
6
Views
4K
  • · Replies 46 ·
2
Replies
46
Views
7K
  • · Replies 5 ·
Replies
5
Views
2K
  • · Replies 4 ·
Replies
4
Views
3K
  • · Replies 23 ·
Replies
23
Views
5K
  • · Replies 9 ·
Replies
9
Views
3K