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Searching for New Exotic Physics at the LHC

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Presentation on theme: "Searching for New Exotic Physics at the LHC"— Presentation transcript:

1 Searching for New Exotic Physics at the LHC
a.k.a. Searches Beyond Supersymmetry Dave Charlton University of Birmingham Before, Behind and Beyond the Discovery of the Higgs Boson Royal Society, January 2014

2 Menu Why search for exotic physics? Simple event types – “bump hunting” Top as a probe Long-lived particles Dark matter Conclusions

3 Simple Event Types “Bump Hunting”

4 m(ee)=1.54 TeV

5 m(μ+μ−)=1.82 TeV

6 Dilepton resonances Model Mass limit (95% CL) Z'SSM 2.96 TeV Z'(ψ) 2.60 TeV Z'SSM 2.86 TeV Z'(E6 models) TeV G*(k/MPl=0.1) 2.47 TeV CMS ATLAS excluded Convert to lower mass limits for specific models In these models, mass of a new resonance must be more than 2-3 TeV Upper limits placed on rate of events (cross-section times branching ratio σ∙B(X→ℓℓ) at 95%CL) ATLAS-CONF Next step: 13 TeV LHC operation – mass reach will ~double

7 High-mass eeγ event

8 W' decaying to leptons Simplest case: W' → ℓν
Single high-pT lepton and Etmiss Again, no excess above backgrounds observed Combining e,μ channels, SM-like W' excluded by CMS for m(W') > 3.35 TeV (95% CL) CMS PAS EXO

9 Event selected in the W'→ℓν analysis, with mT=2.3 TeV

10 Searches in dijets CMS PAS EXO Inclusive dijet mass spectrum – extends up to 5 TeV! Fit with smooth function, look for resonances Limits on many models: string resonances, excited quarks, axigluons, colorons, s8 resonances, E6 diquarks, W' and Z' bosons, and Randall-Sundrum gravitons, up to 5 TeV 5 TeV Further searches in: dijet final states, look at angular distributions in the detector, look at b-tagged jets; multijet topologies searching for 3-jet resonances … …

11 Top as a Probe

12 High transverse momentum top quarks
b W− q q′ jet t b W− q q′ jet High transverse momentum top quarks Low pT Common experimental challenge for searches for heavy particles decaying to top quarks – identification of high-pT tops At high-pT, the top decay products can merge into a single “fat” jet t merged jet High pT Sophisticated “jet substructure” techniques to identify these

13 Search for X → tt Search for a heavy particle decaying to tt
Both semileptonic (tt → bℓvbqq') and hadronic (tt → bqq'bq''q''') decays Search both for resolved and merged jets → extend to very high momentum top quarks ATLAS-CONF Phys Rev Lett 111 (2013)

14 Candidate tt event with m(tt)=2.6 TeV

15 New heavy quarks (“vector-like”)
New heavy quarks (T, B): decay modes T → bW, T → tZ, T → tH B → bZ, B → tW, (B → bH) arXiv: Several event signatures: Single lepton plus jets/ETmiss Same- and opposite-sign dileptons plus jets/ETmiss Trileptons plus jets/ETmiss Use b-tagging to improve signal/background Specially constructed discriminant

16 Put all the information together – complex multidimensional exclusion
Vector-like quarks Put all the information together – complex multidimensional exclusion

17 Combining all channels analysed, CMS obtain lower mass limits of
Vector-like quarks Combining all channels analysed, CMS obtain lower mass limits of m(T) > GeV (95% CL) m(B) > GeV (95% CL) CMS PAS B2G arXiv:

18 Long-lived Particles

19 Dark Matter

20 TeV TeV

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