ZZ 4l measurement with the first ATLAS data

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ZZ 4l measurement with the first ATLAS data XXVIII PHYSICS IN COLLISION Perugia, Italy, 25-28 June 2008 For the ATLAS collaboration: Ilektra A. Christidi Aristotle University of Thessaloniki, Greece

Overview Work done for the Computing System Commissioning (CSC) note Diboson physics studies with the ATLAS detector, using CSC simulated data. Analysis: Muon & electron selection Lepton pairing and cuts on pairs Results Triple Gauge Coupling (TGC) limits Conclusions

Motivation SM cross section not measured yet Irreducible background to H 4l Develop tools for detector calibration using Z 2l Beyond the SM: Triple Gauge Couplings (TGCs) 3 event topologies: 4μ, 4e, 2μ2e Backgrounds: Zbb(bar), tt(bar) Channel ZZ->4l Zbb(bar) tt(bar) MC samples used: Generator Events Filter eff. x-sec 0.219 159fb Pythia 43000 0.009 52pb Acer/Pythia 313689 0.007 833pb MC@NLO/Jimmy 152701 K factor 1.35 1.42 -

The ATLAS detector

Preselection cuts Muons Combined Track (both in Inner Detector and Muon Spectrometer) OR Standalone Track (only in MS no ID for η >2.5) chisq/dof < 15 on match chisq/dof < 15 on fit Pt > 6 GeV/c, η <2.7 Electrons Reconstructed as an electron or both as an electron and a soft electron, by the respective algorithms 0.5 < E/P < 3.0 Pt > 6 GeV/c, η <2.5 Create same flavor, opposite charge pairs with lepton ΔR>0.2

After preselection: Pt At least one lepton in each pair with Pt > 20 GeV/c 4μ 4e ZZ 4l signal Zbb bg ttbar bg

After preselection: Isolation Electron: Cuts on the shower shape in the electromagnetic calorimeter Muon: Isolation Ratio < 0.2 (energy in a cone of ΔR = Δφ 2 Δη 2=0.4 around the muon, divided by Et) ZZ 4l signal Zbb bg ttbar bg

2l invariant mass ZZ: m of both lepton pairs between 70 and 110 GeV/c ZZ*: m(pair1) between 70 and 110 GeV/c, m(pair2) > 20 GeV/c

Final 4l Invariant Masses: ZZ normalized to 10fb ¹ 4e 4μ 2μ2e

Final 4l Invariant Masses: ZZ* normalized to 10fb ¹ 4e 4μ 2μ2e

Efficiency summary Signal Zbb tt

Results: signal/bg Results below are normalized to 1fb ¹ sg/bg = significance = 8.7 6.6 66.5 7.7 Where significance = sg/ bg, and the 95% Poisson limit for 1 and 0 events respectively is used for background

Systematic errors From MC and data Theoretical uncertainties: PDFs, QCD corrections (scaling uncertainty for NLO calculations): 3.4-6.2% (run MC with different structure functions/scale values) Luminosity: ~5% (Tevatron: 6.5% at 0.3 fb ¹, and got less with more accumulated luminosity) Trigger & Lepton identification efficiency: 2-3% (MC data with pileup and cavern backgrounds, OR real data with tag-andprobe method with Z 2l decays) Jet & lepton energy scale: 2-3% (from WW & WZ Boosted Decision Trees study) Background estimate: ~2% (mainly from lepton identification)

TGCs: the principle i s M 2 V V α μβ β μα Γ αβμ = [ f P g P g f V ε μαβρ q 1 q2 ρ ] ZZV 4 5 M2 Z V = Z, γ P. Ward et al., University of Cambridge f V = f V =0 at tree level in the SM 4 5 Z, f Z,f γ, f γ f 4 parameters accessible with ZZ 4l: 4 5 4 5 4 observables change with anomalous TGC: cross-section vs Pt(Z), M(ZZ), lepton angle, Z angle The following results are with only Pt(Z) distributions

TGCs: the method In collaboration with P. Ward et al., University of Cambridge Use LO Baur-Rainwater (BR) MC to generate Pt(Z) distributions for different f V i Fit cross-section to quadratic function of f V in bins of Pt(Z) i Correct for NLO effects with the ratio of full NLO MC to the Standard Model ( f V =0) BR one i Find efficiency from full MC (events after all cuts/truth events)

TGCs: likelihood Expected events = BR x-section NLO correction efficiency luminosity Generate fake event samples based on this expectation for signal and Zbb background Binned Likelihood in each Pt(Z) bin: V with one free parameter ( ν s f i ). In all bins V Minimizing this, we get the most likely f value and the CLs. i

TGCs: results 95% CL intervals at 10 fb ¹

Conclusions Baseline ZZ 4l analysis done Signal expectation at 1 fb ¹: 13.3 ZZ, 16.5 ZZ* events, with at least an order of magnitude lower background Systematic errors need to be better understood TGC limit measurement is promising to improve the LEP limits with the first 10 fb ¹ of data Many ideas for improvements/optimizations

Extras

Single lepton effic./fakes muons: electrons: efficiency = 0.90 efficiency = 0.76 fake rate = 0.003 fake rate = 0.001

Future plans Use also low-pt muons (only ID track and MS hits) Look into more ways to reduce bg Vertexing/IP for Zbb Et(miss) for tt Assess & correct lepton-to-z mis-assignment preliminary study shows ~4% mis-assignment! Tune cuts for ZZ* 4l? (relevant for low Higgs mass) Refine Z mass cut for on-shell Z: constrained fit? Calculate ΖΖ 4l background to H 4l from data For TGCs: Use the rest of the observables to improve limit (advantage over the ZZ llνν channel) Multi-dimensional fits?