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New Physics at a TeV and the LHC – II & III

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Presentation on theme: "New Physics at a TeV and the LHC – II & III"— Presentation transcript:

1 New Physics at a TeV and the LHC – II & III
Higgs and New Physics Searches at the LHC Sreerup Raychaudhuri Tata Institute of Fundamental Research, Mumbai, India IPM String School (ISS 2009), Tehran, Iran April 17, 2009

2 Significance of the TeV energy scale:
top-down approach : GUT or stringy unification must have low energy consequences; high scale SUSY will have low energy manifestations, extra dimensions will become accessible at high enough energies bottom-up approach : hierarchy problem, neutrino masses, GUT evolution aesthetic approach : 18 free parameters in the SM no QCD-EW unification desert scenarios

3 Capabilities of the LHC
Cannot do a blind search… All important final states require a trigger

4 LHC has severe limitations….
Huge QCD backgrounds… especially if looking for hadronic final states Cannot see very soft pT jets/leptons/photons LHC has severe limitations….

5 Sure shots : Can determine t quark properties to precision Can find the Higgs boson of the SM (if it exists) Can find a SUSY signal if kinematics permits Can find a resonant new state Less sure : Can measure Higgs boson couplings Can measure SUSY parameters Can discover exotics, e.g. gravitons, monopoles…

6 How are we so sure?

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16 RG evolution of mSUGRA spectrum
11 RG evolution of mSUGRA spectrum

17 12 Present status of MSSM parameter space

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