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Studies of J et S hapes and S ubstructure with ATLAS Adam Davison University College London

Studies of J et S hapes and S ubstructure with ATLAS Adam Davison University College London. ATLAS. Recorded ~5 fb -1 of 7 TeV pp collisions from the LHC Highly granular calorimetry (down to 0.025x0.025 in η-φ ). Jets at ATLAS. At the LHC jets are everywhere

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Studies of J et S hapes and S ubstructure with ATLAS Adam Davison University College London

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  1. Studies of Jet Shapes and Substructure with ATLASAdam DavisonUniversity College London

  2. ATLAS • Recorded ~5 fb-1 of 7 TeVpp collisions from the LHC • Highly granular calorimetry (down to 0.025x0.025 in η-φ)

  3. Jets at ATLAS • At the LHC jets are everywhere • ATLAS primarily uses anti-kt jets with R = 0.4 and 0.6 • Other algorithms available for specialised needs • Rich series of jet physics publications from ATLAS already • Inclusive jets, dijets, multijets, b-jets, azimuthal correlations etc…

  4. Inside a Jet • Jets can contain a lot of complex physics • Non-perturbative effects like fragmentation and hadronisation • Hard process, colour connections, UE, pile-up • Massive particle production (b, c, W, Z, top etc…) • Measurements of the internal structure of jets can help us test models and tunes for all of these • Good models of all of these a necessity for BSM searches

  5. Jet Shapes • Jet shapes are the classic test of the internals of jets • Measure the fraction of a jet’s pt which is within an annulus • Formally, measure the quantity: pT in annulus pT of jet

  6. Jet Shapes 2.4.2 • Results released 2010, now published: • Phys.Rev. D83 (2011) 052003 • More recently, newer tunes tested • ATL-PHYS-PUB-2011-010

  7. Fragmentation • Can also study the distribution of charged particles the jet (jet) a track (ch) • Distribution of energy parallel or transverse to jet axis:

  8. Eur. Phys. J. C 71 (2011) 1795 Fragmentation • Distributions are reasonably well modelled

  9. Jet Mass and Substructure • Jets are 4-vectors, for example (E/pT, η, φ, m) • Of these, mass is probably the least studied • At the LHC, lots of interest in jet mass and substructure • Especially large radius jets • Jets can contain boosted W, Z, top … • … and potentially new physics • Measurements targetted at this ATLAS-CONF-2011-103

  10. New Results! Jet Mass and Substructure • Looking at Cambridge-Aachen R=1.2 and anti-kt R=1.0 • Jet mass measured for jet pt of 200 – 600 GeV • Systematics determined in-situ using inner-detector track jets • Herwig++didn’t describe this terribly well in version 2.4.2 http://arxiv.org/abs/1203.4606

  11. Jet Mass and Substructure • Also look at application of a substructure procedure: Splitting and filtering a la PRL 100, 242001 (2008) Less sensitive to soft physics, observe better agreement than in plain jet mass http://arxiv.org/abs/1203.4606

  12. Jet Mass and Pile-up • Looking at mean mass vs. pile-up • Splitting/filtering reduces dependence significantly http://arxiv.org/abs/1203.4606

  13. Jet Mass and Substructure • Also look at kT splitting scales (aka y-scales, d12) • Measure of scale at which a jet breaks into two subjets

  14. Jet Mass and Substructure More like 3 subjets than 2 • n-subjettiness, new variable (arXiv:1011.2268 (2011) Thaler, Tilburg) Sum distances from constituents to 2 or 3 ktsubjet axes Take ratio of sums http://arxiv.org/abs/1203.4606

  15. Conclusions • ATLAS has made many measurements of internals of jets • Jet shapes (Phys.Rev. D83 (2011) 052003) • Jet fragmentation (Eur. Phys. J. C 71 (2011) 1795) • Jet mass and substructure variables (arxiv:1203.4606) • All available in HepData(in a week-ish for jet mass) • Variables designed for new physics searches appear to be well modelled generally by Monte Carlo • More to come with 8 and 14 TeV

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