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How exactly will LHC detect superpartners? Presumably they will have higher mass, are there other ways to detect them?
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.
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.
Limitations include the dependence on specific theoretical models and the unresolved nature of certain measurements and assumptions regarding particle interactions and properties.
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).
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).