How exactly will LHC detect superpartners?

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Discussion Overview

The discussion centers on how the Large Hadron Collider (LHC) will detect superpartners, a concept from supersymmetry, and explores the detection of the Higgs boson and potential evidence for higher dimensions. The conversation includes theoretical models, detection methods, and challenges associated with proving the existence of these particles.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • Some participants propose that the detection of superpartners depends on the model, particularly the Minimal Supersymmetric Standard Model (MSSM), which involves the concept of R-parity.
  • It is noted that in MSSM, Standard Model particles have R-parity +1 while their superpartners have R-parity -1, leading to the lightest supersymmetric partner (LSP) being stable and undetectable, resulting in missing momentum in experiments.
  • One participant questions whether the signature of missing momentum would definitively prove supersymmetry or if it could be attributed to a non-supersymmetric particle with a similar mass.
  • Another participant suggests that proving a particle is a superpartner requires demonstrating a spin difference of 1/2 and verifying that the partners have the same couplings as Standard Model particles.
  • There are references to recent papers discussing potential measurements at the LHC that could support these claims.
  • Regarding the Higgs boson, it is mentioned that decays to two photons provide a clean detection channel, but care must be taken to confirm it is indeed the Higgs boson by measuring its spin and couplings.
  • One participant expresses skepticism about the ability to reconstruct the Higgs potential shape at the LHC.

Areas of Agreement / Disagreement

Participants express multiple competing views on the detection methods and implications of findings related to superpartners and the Higgs boson. There is no consensus on the definitive proof of supersymmetry or the capabilities of the LHC in measuring certain properties.

Contextual Notes

Limitations include the dependence on specific theoretical models and the unresolved nature of certain measurements and assumptions regarding particle interactions and properties.

bananan
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How exactly will LHC detect superpartners? Presumably they will have higher mass, are there other ways to detect them?
 
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It really depends on the model. In models like the (Minimal Supersymmetric Standard Model) MSSM, there is a quantity called R-parity. Each Standard Model particle has R-parity +1 and each partner has R-parity -1. R-parity is conserved in interactions which means that the lightest partner (R-parity -1 state) will be stable (since it can only has R-parity +1 states that are lighter).

This Lightest Supersymmetric Partner (LSP) then leaves the detector without being seen. This is a real smoking gun because then the momentum in the plane transverse to the beam will not be conserved by the visible particles (the momentum parallel to the beam isn't either, but this is useless because one doesn't know the initail particle momenta, only their direction).
 
Severian said:
It really depends on the model. In models like the (Minimal Supersymmetric Standard Model) MSSM, there is a quantity called R-parity. Each Standard Model particle has R-parity +1 and each partner has R-parity -1. R-parity is conserved in interactions which means that the lightest partner (R-parity -1 state) will be stable (since it can only has R-parity +1 states that are lighter).

This Lightest Supersymmetric Partner (LSP) then leaves the detector without being seen. This is a real smoking gun because then the momentum in the plane transverse to the beam will not be conserved by the visible particles (the momentum parallel to the beam isn't either, but this is useless because one doesn't know the initail particle momenta, only their direction).

Thanks for the reply.

I guess while we are on subject, how will LHC see the higgs boson, and how could it see higher dimensions if they exist?
 
Severian said:
It really depends on the model. In models like the (Minimal Supersymmetric Standard Model) MSSM, there is a quantity called R-parity. Each Standard Model particle has R-parity +1 and each partner has R-parity -1. R-parity is conserved in interactions which means that the lightest partner (R-parity -1 state) will be stable (since it can only has R-parity +1 states that are lighter).

This Lightest Supersymmetric Partner (LSP) then leaves the detector without being seen. This is a real smoking gun because then the momentum in the plane transverse to the beam will not be conserved by the visible particles (the momentum parallel to the beam isn't either, but this is useless because one doesn't know the initail particle momenta, only their direction).

I wonder whether such a signature would prove SUSY, as opposed to a non-SUSY previously unknown particle with similar mass.
 
Yes, to prove it is SUSY you really need to do two things:

1. Prove the particles differ by spin 1/2.
2. Prove that the partners have the same couplings as the SM ones.

I have seen it claimed that 1 is only possible at a linear collider, but there have been some papers more recently on this, e.g. http://arxiv.org/abs/hep-ph/0605067 and http://arxiv.org/abs/hep-ph/0605286, which discuss measurements at the LHC.

As for the Higgs boson, there are various signals. For example, Higgs decays to two photons are nice because the diphoton invariant mass will give a peak at exactly the Higgs boson mass. This is a rather clean channel, and as soon as it is seen I am sure there will be a discovery announcement.

However, again, one has to be careful to make sure it is a Higgs and not something else. To do this, you really need to measure its spin (to see it is a scalar) and its couplings (to show they are proportional to the mass of the particle it couples to). Eventually if you can measure itself couplings you can actually reconstruct the shape of the mexican hat potential of the Higgs boson. Unfortunately this last thing won't be possible at the LHC.
 
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