Central Exclusive DiMuon Production

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Presentation transcript:

Central Exclusive DiMuon Production Ronan McNulty (UCD Dublin) On behalf of the LHCb collaboration SM@LHC, Durham, 11th-14th April 2011 Ronan McNulty, SM@LHC, Durham 11-14 April 2011

Ronan McNulty, SM@LHC, Durham 11-14 April 2011 Motivation Usually proton collisions produce very many final state particle because the gluon is a coloured object. But if a colourless object is exchanged….. Results can be related to HERA and Tevatron Understand QCD in a clean environment Unambiguous evidence for pomeron. Search for odderon Constrain unintegrated parton distributions at very small x (2x10-6) Search for saturation effects Ronan McNulty, SM@LHC, Durham 11-14 April 2011

Central Exclusive Production y=-10 y=-2 y=0 y=2 y=10 Elastic Scattering Single Diffraction Double Diffraction Central Exclusive Production (elastic) Central Exclusive Production (inelastic) Ronan McNulty, SM@LHC, Durham 11-14 April 2011

LHCb: a forward spectrometer y Tracking Stations Interaction Point Muon Chambers 250mrad 10mrad VELO l 20m z Magnet RICH detectors ECAL HCAL Ronan McNulty, SM@LHC, Durham 11-14 April 2011

Use of backwards tracks Clearly not exclusive Ronan McNulty, SM@LHC, Durham 11-14 April 2011

Trigger on two muons and <20 SPD hits Requiring a gap, there is evidence for central exclusive production decaying to two muons. Ronan McNulty, SM@LHC, Durham 11-14 April 2011

Simple Selection Criteria No backward tracks (gap of ~2 units of rapidity) Precisely two forward muons No photons (for J/psi and diphoton process) One photon (for ChiC analysis) pT of dimuon <900 MeV (<100MeV for pmmp). Ronan McNulty, SM@LHC, Durham 11-14 April 2011

Ronan McNulty, SM@LHC, Durham 11-14 April 2011 Dimuon Mass Spectrum after trigger demand gap Ronan McNulty, SM@LHC, Durham 11-14 April 2011

Ronan McNulty, SM@LHC, Durham 11-14 April 2011 J/ψ and ψ’ No backward tracks Precisely two forward muons No photons Ronan McNulty, SM@LHC, Durham 11-14 April 2011

J/ψ and ψ’: Number of Photons Estimated feeddown from Chi_c Ronan McNulty, SM@LHC, Durham 11-14 April 2011

J/ψ and ψ’: Number of Tracks ψ’ feeddown Tempting to fit the background under the peak using straight line/exponential. Better if we can understand the physics giving background. Ronan McNulty, SM@LHC, Durham 11-14 April 2011

Inelastic backgrounds Ronan McNulty, SM@LHC, Durham 11-14 April 2011

Fit elastic and inelastic components Estimate purity below 900 MeV to be 80+-3 % Ronan McNulty, SM@LHC, Durham 11-14 April 2011

J/ψ Non-resonant background & misid This is not background subtracted ! Ronan McNulty, SM@LHC, Durham 11-14 April 2011

ψ’: Non-resonant backgrounds & misid Ronan McNulty, SM@LHC, Durham 11-14 April 2011

Ronan McNulty, SM@LHC, Durham 11-14 April 2011 pp->pmmp No backward tracks Precisely two forward muons. mmm>2.5 GeV No photons Ronan McNulty, SM@LHC, Durham 11-14 April 2011

Fit elastic and inelastic components Shape for inelastic events Note: this time we have simulation that predicts the shape for the three contributions. Fit to signal events Background shape from data Signal shape from simulation. Ronan McNulty, SM@LHC, Durham 11-14 April 2011

Ronan McNulty, SM@LHC, Durham 11-14 April 2011 No backward tracks Precisely two forward muons Precisely one photon Ronan McNulty, SM@LHC, Durham 11-14 April 2011

χc: DiMuon Invariant Mass About half the background that was observed in the exclusive J/ψ analysis (since no continuum process). Ronan McNulty, SM@LHC, Durham 11-14 April 2011

χc: DiMuon+Photon Invariant Mass (Caveat: Inelastic contribution appears to be much larger than for J/ψ) Ronan McNulty, SM@LHC, Durham 11-14 April 2011

Cross-section calculations σ=(pN/ε) / L ε: Trigger, tracking, photon & selection efficiencies are estimated from simulation, with size of systematics taken from data/simulation agreement. p: Feed-down for ψ’, χc subtracted. Uncertainty on fit to pT spectrum taken as systematic on inelastic contribution. L: Analysis only uses single-interaction events. Need to know average number of pile-up interactions. Currently translates into 20% uncertainty on L. Ronan McNulty, SM@LHC, Durham 11-14 April 2011

Ronan McNulty, SM@LHC, Durham 11-14 April 2011 Summary Ronan McNulty, SM@LHC, Durham 11-14 April 2011

Ronan McNulty, SM@LHC, Durham 11-14 April 2011 Comparison to Theory Starlight (Klein & Nystrand) 292 pb SuperChic (Harland-Lang, Khoze, Ryskin, Stirlin) 330 pb Motyka & Watt 330 pb Schäfer & Szczurek 710 pb J/ψ: 474 +-103 pb ψ’: 12.2 +- 3.2 pb Starlight (Klein & Nystrand) 6 pb Schäfer & Szczurek ~ 17 pb Starlight (Klein & Nystrand) 0.16 Schäfer & Szczurek ~ 0.2 HERA: 0.166 +- 0.012 (lower √(p) ) CDF: 0.14 +- 0.05 (lower √(p) ) σ(ψ’)/σ(J/ψ): 0.20 +- 0.03 χ0: 9.3 +- 4.5 pb χ1: 16.4 +- 7.1 pb χ2: 28.0 +-12.3 pb SuperChic: 14 pb 10 pb 3 pb pμμp: 67 +- 19 pb LPAIR (J. Vermaseren) 42 pb Ronan McNulty, SM@LHC, Durham 11-14 April 2011

Ronan McNulty, SM@LHC, Durham 11-14 April 2011 Summary First Observation of CEP at LHC First separation of χc spin states in CEP Good agreement with theory predictions Consistency with HERA and CDF results. Ronan McNulty, SM@LHC, Durham 11-14 April 2011