2. Yet another statistically insignificant hint of New Physics or ZZ cross section measurement with 4.6 fb -1 of 7 TeV ATLAS data arxiv:1211.6096, submitted to JHEP Alexandru Dafinca, David Hall, Roger Naranjo, Edgar Valencia, Ivonne A. Maldonado Cervantes, Gonzalo Diaz, Jose La Rosa, Margot Delgado de la Flor, Alejandro de la Puente, Estefania Coluccio Leskow, Gilberto Chavez Meza, Vanessa Theodoro, Gibraham Napoles, Andrés Melo

3. Motivation Tests electroweak physics Background to Higgs search Set limits on anomalous triple gauge couplings (aTGC) neutral TGCs not in SM ATLAS diboson x-sections measured high at 7 TeV 17/03/20132CLASHEP-13, Arequipa, Peru

4. The ATLAS detector Inner detector within solenoid magnet pixels for vertex location silicon detector tracks charged particles |η| < 2.5 EM & hadronic calorimeters measures energy deposited |η| < 4.9 Muon spectrometer toroidal magnet tracks muons |η| < 2.7 η = - ln tan(θ/2) LevelRate Initial40 MHz L1100 kHz L23 kHz L3200 Hz 3-level trigger system 17/03/20133CLASHEP-13, Arequipa, Peru

5. Analysis overview pp ZZ ZZ ( * ) ZZ νν Both on-shell ZZ One off-shell ZZ * ChannelClassificationm ll ZZ On-shell66 – 116 GeV Off-shell> 20 GeV ZZ νν 76 – 106 GeV 17/03/20134CLASHEP-13, Arequipa, Peru Identification of Z bosons Resolve ambiguous cases by selecting the combination that minimises the sum of |m ll - m Z | for the two pairs

6. ZZ ( * ) event selection pass electron or muon trigger exactly 4 isolated leptons with p T > 7 GeV – e + e - e + e -, μ + μ - μ + μ -, e + e - μ + μ - require at least one muon with p T > 20 GeV or electron with p T > 25 GeV each same-flavour, opposite-charge dilepton system forms a Z candidate events sorted into ZZ and ZZ* categories 17/03/2013CLASHEP-13, Arequipa, Peru5

7. ZZ νν event selection 17/03/2013CLASHEP-13, Arequipa, Peru6 pass electron or muon trigger exactly 2 isolated leptons with p T > 20 GeV: e + e -, μ + μ - Z candidate in mass window veto event if jet p T > 25 GeV (reduce top background) discriminating MET variables to reduce Z+jets bkg:

8. How to get an inclusive σ from data 17/03/2013CLASHEP-13, Arequipa, Peru7 MC Inclusive Data Fiducial region (truth level) Signal region (reco. level) measure σ fid – cross section measured within a restricted (kinematic and geometric) phase space σ total – cross section extrapolated to total phase space

9. Systematic uncertainties 17/03/2013CLASHEP-13, Arequipa, Peru8 But how do we obtain N bkg ?

10. give rise to lepton-like jets (lepton candidates failing isolation criteria) background:j and jj with mis-ID jet(s) define measure f based on lepton-like jets in a sample of Z+jets in data/MC in bins of p T total number of expected background events: Backgrounds to ZZ ( * ) 17/03/2013CLASHEP-13, Arequipa, Peru9 Leptons from HF decay can pass ID cuts Other mis-ID sources: leptons from π 0, K decay jets misidentified as leptons

11. Backgrounds to ZZ ( * ) 17/03/2013CLASHEP-13, Arequipa, Peru10 Expected number of background events < 1 for ZZ

12. Backgrounds to ZZ νν tt, WW, Wt and Z ττ – two true isolated leptons with missing p T extrapolate from a control sample of eμ events WZ – 3 lepton final state, but one lepton is not identified estimated using MC validated using a control region of 3 high-p T leptons Z+jets – may have missing p T due to mis-measurement of jet p T estimated using high-p T γ +jets events Z+jets, W+jets, Z γ, W γ – jet or γ mis-identified as lepton use the matrix method to estimate the fraction of events in the signal region containing at least one fake lepton 17/03/2013CLASHEP-13, Arequipa, Peru11

13. 17/03/2013CLASHEP-13, Arequipa, Peru12 Backgrounds to ZZ νν Distributions in signal region using background estimations in previous slide

14. Cross section results Measured (fb)NLO prediction (fb) 17/03/2013CLASHEP-13, Arequipa, Peru13 maximum likelihood fitting method treat systematics as nuisance parameters single Gaussian across channels for correlated uncertainties

15. aTGC limits 17/03/2013CLASHEP-13, Arequipa, Peru14 CP conserving CP violating aTGCs described by 4 parameters f V i (with f V i = 0 in SM) aTGCs produce longer tail in p T Z spectrum fit p T Z distribution limits set using maximum profile likelihood ratio 95% CL

16. Conclusions total and fiducial ZZ cross sections measured with full 2011 dataset used ZZ ( * ) and ZZ νν decay channels statistically consistent with SM NLO prediction, although measured value is slightly higher – analysis recently performed in 4 channel with 20 fb -1 of 8TeV data: ATLAS-CONF-2013-020ATLAS-CONF-2013-020 17/03/2013CLASHEP-13, Arequipa, Peru15

17. 17/03/2013CLASHEP-13, Arequipa, Peru16

18. We thank our sponsors 17/03/2013CLASHEP-13, Arequipa, Peru17

19. Backup slides