*if* the higgs can not be found

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In summary: So while I think the likelihood of the Higgs is high, we can't say that the SM is a swiss cheese and that the only thing keeping it together is the Higgs. In summary, the thread has been moved from astrophysics to particle physics, and the meaning of the phrase "Standard Model" is different. The Standard Model is the theory of the electroweak and strong forces. Quarks, gluons, and all that...
  • #1
wolram
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Is there a model that will permit a higgs-less model, without to much adjustment to the standard model ?
 
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  • #2
why has this question been moved,after all it is to to the heart of astro phytsics
 
  • #3
Perhaps i should also ask about the super symetric particles that have
also not been found.
 
  • #4
wolram said:
why has this question been moved,after all it is to to the heart of astro phytsics

But astrophysics is not the field in which the answer to the question should be found, if it exists. This is.
 
  • #5
The Higgs is extremely important in the Standard Model. All the gauge bosons and most of the fermions are protected from having direct mass terms by gauge invariance. The only exception is the right handed neutrinos which are gauge sterile and hence can have a direct mass term in addition to a coupling to the Higgs. Everything else gets its mass from the Higgs vacuum expectation value. In particular, the Goldstone modes associated with the electroweak symmetry breaking are absorbed by some of the gauge bosons. We do observe massive fermions and massive gauge bosons, and we don't observe massless scalar fields. So the point is that Higgs is critical the Standard Model we all know and love. Of course, just because the Higgs isn't found at the LHC doesn't mean it doesn't exist. The theory doesn't predict the mass of the Higgs, and while many researchers have convinced themselves that the Higgs must be somewhere near, it is entirely possible that the Higgs sector could be more complicated than we suspect. I can't say exactly what the full gamut of alternatives is, but I can tell you that the Higgs is very important and so a major modification would be necessary.
 
  • #6
Thankyou Physics Monkey, as a pleb, i find the standard model seems to be
a swiss cheese, the only things going for it is a contrived Hubble constant, and an untestable red shift, the SM still needs dark energy, dark matter,
super symetric particles, if any thing the SM should be moved to Ivans
forum.
 
  • #7
wolram said:
Thankyou Physics Monkey, as a pleb, i find the standard model seems to be
a swiss cheese, the only things going for it is a contrived Hubble constant, and an untestable red shift, the SM still needs dark energy, dark matter,
super symetric particles, if any thing the SM should be moved to Ivans
forum.


Umm, one problem with the thread being moved from astrophysics to particle physics is that the meaning of the phrase "Standard Model" is different. Physics Monkey isn't talking about the big bang and inflation, he's talking about the theory of the electroweak and strong forces. Quarks, gluons, and all that...

I am a skeptic about supersymmetry myself, and experiments at Tevatron have put it under the gun for likely discoveries at LHC, but sheer speculation it isn't.
 
  • #8
A small correction to what PhysicsMonkey said - if the only fundamental particles are those we know of, plus the Higgs, then it *will* be found at the LHC. This is due to the fact that, in the SM, there is an upper bound to the Higgs mass, and that is below the highest mass Higgs the LHC can see. Now, if there's new physics such as SUSY, then there are ways for the Higgs to hide (although generally not by being too heavy, the new physics can sometimes produce enough extra background that the Higgs signal is lost).

To answer the original question: there have been proposals for models of Electroweak symmetry breaking that do not involve the Higgs. The most famous is called Technicolor, which for many years was the main competitor to SUSY for the correct theory of physics at the TeV scale. In this model the role of the Higgs is shifted to a set of new gauge bosons and fermions that are strongly interacting. Experiments at the LEP accelerator at CERN have disfavored Technicolor models, but have not excluded the idea, and a fair bit of work is ongoing in that direction.
 
  • #9
Hi BenLillie,

I feel the silly need to defend my post, so here goes. I did in fact say that most physicists expect to find the Higgs at LHC unless the Higgs sector is more complicated i.e. supersymmetry. The Standard Model, in and of itself, doesn't necessarily constrain the Higgs mass all that closely, yes? When we say that the Higgs *will* be found, what we mean is that assuming the Standard Model is valid as we know it now and using precision electroweak data we put the Higgs mass at less than 190 GeV (if memory serves, please correct me if I have the latest number wrong) with 95% CL. My only point is that this is not quite certainty especially since it based on a number of assumptions that we expect to be modified anyway.

On a less defensive note, as someone who is interested in effective theories of QCD, I have a special place in my heart for technicolor even if it doesn't pan out. Chiral perturbation theory is just too cool.
 
  • #10
No need to worry, it's a minor point :)

But, the LHC can, in fact, find a Standard Model Higgs up to masses of about 1 TeV. There is a bound coming from unitarity of longitudinal W scattering that requires the Higgs mass to be < 850 GeV, hence the statement that the LHC will find a SM Higgs. You're absolutely correct that the precision electroweak bounds are not airtight, but the unitarity bound is very solid.
 
  • #11
No problem, this isn't my area of expertise, so I'm happy to hear from someone else on the matter. Regarding the unitarity bound, perhaps you can clarify something for me. I understood that the bound you quote was perturbative, and that if you summed to all order in the Higgs coupling then you got a true bound which was a bit over a TeV so that there was still a loophole there at least as far as the LHC was concerned.
 
  • #12
Unitarity bounds are pretty strong, except that you can nearly always add extra degrees of freedom to push the bound around. So assuming the vanilla SM, we must see something Higgs like, otoh if we see extra stuff (not necessarily supersymmetry, but instead extra fields) then all bets are off, you would have to redo the computation.

Fortunately if we see new physics, it is almost guarenteed to be more interesting and informative than if we simply see a 120 GeV Higgs scalar and nothing else.
 
  • #13
Haelfix is absolutely correct. Also, the fact that you have to introduce new degrees of freedom to evade the unitarity bound leads to one of the famous "no lose theorems" for the LHC. Basically, if the Higgs isn't there to be found, then there must be something else that couples to Ws and Zs with a mass not much above 1 TeV. Obviously, that's not an airtight argument that the LHC can discover the new states, but in every model I've seen *something* is visible at the LHC.

I've never seen an all-orders calculation of longitudinal gauge boson scattering, and I'd be surprised if it was possible. I know the one-loop correction has been done, but I don't remember the direction of the shift, only that it didn't change the argument qualitatively. At the very high end there could be a region that's invisible, that's believeable.
 
  • #14
I definitely agree with both of you, and I'm reminded of the old Fermi theory of weak decays where the violation of unitarity was a signal of the new physics of the W and Z. I know Haelfix and I have talked about this before, how unitarity is a very powerful tool. Anyways, hopefully we will get much more than we bargained for, just to keep things interesting. :wink:
 
  • #15
@ Physics Monkey...

You are saying about the full calculation of the WW scattering... But as long as we are in the perturbative region, I don't think it's necessary... See, in the tree level amplitude we have terms of order of λ, (apart from
the constant terms, irrelevant at high energies). Now, this term cannot be modified by any λ^2 terms or the higher order terms... What we need is, the divergence will be canceled order by order... So, I think there should be a bound From each Order of λ... Of course, it is good to keep an eye on each order, but that will be
a tedious work... What I mean to say is that, one may have better bounds from higher order calculations.. but
the bound from tree level amplitude will not be modified...

Sorry for my english... And thank you guys, for such kind of threads...
 
  • #16
This thread is 5 years old.
 

1. What would happen if the Higgs boson cannot be found?

If the Higgs boson cannot be found, it would challenge our current understanding of the Standard Model of particle physics. This would require scientists to reconsider and potentially revise their theories and models.

2. Would the discovery of the Higgs boson have any practical applications?

The discovery of the Higgs boson would not have any immediate practical applications. However, it would deepen our understanding of the fundamental building blocks of the universe and could potentially lead to new technologies in the future.

3. How would the absence of the Higgs boson affect our understanding of the universe?

The Higgs boson is a crucial piece of the Standard Model, which is the current theory that explains the fundamental particles and forces of the universe. Without it, our understanding of how particles acquire mass and the structure of the universe would need to be reevaluated.

4. Would the absence of the Higgs boson disprove the existence of dark matter?

No, the Higgs boson is not directly related to the existence of dark matter. Dark matter is a hypothetical substance that is thought to make up a large portion of the universe's mass, but its exact nature is still unknown.

5. How would the search for the Higgs boson continue if it cannot be found?

If the Higgs boson cannot be found at the current energy levels of the Large Hadron Collider, scientists may continue to search for it at higher energy levels or through other experiments. They may also explore alternative theories that do not require the existence of the Higgs boson.

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