Testability of GUTs at the LHC

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Discussion Overview

The discussion centers on the potential for experiments at the Large Hadron Collider (LHC) to test Grand Unified Theories (GUTs) in particle physics. Participants explore whether the LHC can rule out or verify various proposed GUTs, considering the energy scales involved and the types of signatures that might be observed.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Exploratory

Main Points Raised

  • One participant expresses skepticism about the LHC's ability to test GUTs, noting that the GUT scale is typically at energies near the Planck scale, far beyond the LHC's reach.
  • Another participant argues that certain GUT decompositions could lead to observable phenomena, such as new neutral current processes (Z primes) or additional gauge bosons (W primes), which could be searched for at the LHC.
  • Some participants mention the challenge of distinguishing GUT signals from non-GUT models, suggesting that while some discoveries might be possible, the specifics may remain elusive.
  • There is a discussion about the potential to measure properties of any new resonances found, which could provide constraints on various models, although a linear collider might be necessary for deeper probing.

Areas of Agreement / Disagreement

Participants express differing views on the LHC's capability to test GUTs, with some believing that certain signatures could be detected while others remain doubtful about the collider's effectiveness in illuminating GUT processes. No consensus is reached on the overall potential of the LHC in this context.

Contextual Notes

Participants highlight the limitations of current experimental setups and the high energy scales associated with GUTs, as well as the complexities involved in distinguishing between GUT and non-GUT models.

Orbb
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Hello,

my understanding of particle physics is very limited. I know that several GUTs involving various symmetries have been proposed. My question is, wether experiments at the LHC can help to rule out or even verify some of the proposed GUTs? Maybe someone has some specific answers. Thank you!
 
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Doubtful, the usual hypothetical GUT scale is at very high energies, near the Planck scale, many orders of magnitude away from what the LHC probes. The best you can do is get better experimental precision on the standard coupling constants (Electroweak, Strong) that way we can refine the interpolation when we run them down to that scale to see if they unify. Right now, they nearly hit but not quite (with Supersymmetry its even closer).

Barring that, we need better precision on the bounds of potential proton decay (a typical prediction of GuTs is that indeed protons do decay after a very long time) but the LHC won't help us there directly either.

Still sometimes there are roundabout ways of getting there, depending on which physics we see or don't see but I wouldn't count on it.
 
I respectfully disagree with the post above. Many GUTs include decompositions such as (and as a very simple example):

[tex] SO(10) \to SU(5) \otimes U(1)_{GUT} \to SU(3) \otimes SU(2) \otimes U(1)_{Y} \otimes U(1)_{GUT}[/tex]

The new U(1) would exhibit itself as a new neutral current process (so called Z primes). There are further decompositions where one finds new SU(2) x U(1), implying W primes as well as Z primes.

There are people actively looking for these things in various channels of potential interest, and some models provide striking signatures. Now, we will either make some exceedingly exciting discoveries or rule out certain models and model parameters.
 
I agree that the discovery of say tev neutral current processes *might* shed some light on GUT processes if we are really lucky, but its far more probable a hadron collider won't be able to illuminate the specifics. The inverse problem is in full effect there since a number of potential non GUT models contain them. Afaik, they are hard to disentangle.
 
Haelfix said:
The inverse problem is in full effect there since a number of potential non GUT models contain them. Afaik, they are hard to disentangle.

Depends on just how much you want to disentangle. It's fairly easy (given enough integrated luminosity) to measure the spin and couplings of any new resonance from the decay kinematics, and this constrains things hugely. I.e. Spin 1 implies a new U(1) like thing, Spin 2 implies (amongst other things) KK models, same-sign events can imply exotic models with doubly-charged resonances etc etc. You can also add in further evidence - displaced decay vertices can imply models with B-L symmetry, boosted decay products can give further handles etc etc.

The argument is, of course, that a linear collider will be needed to really probe any new structure, but we'll definitely be able to say more than 'It's a bump at 1.5 TeV' if we find something.
 

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