Missing Energy and Tau-Lepton Reconstruction in ATLAS

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Presentation transcript:

Missing Energy and Tau-Lepton Reconstruction in ATLAS Stefan Stonjek Max-Planck-Institut für Physik Physics at LHC Seminar 27-May-2008

Stefan Stonjek: Missing Energy and Tau in ATLAS Outline ET,miss Reconstruction algorithms Refinement Performance Tau-jet reconstruction 27-May-2008 Stefan Stonjek: Missing Energy and Tau in ATLAS

Stefan Stonjek: Missing Energy and Tau in ATLAS Why ET,miss and tau ET,miss is vital for almost all physics analyses In particular for new physics New physics is supposed to appear at high ET,miss Tau leptons provide a good handle to new physics Like: H / A → tau + tau Tau decays 35% leptonically (tau → e/μ + neutrino + tau-neutrino) 65% hadronically (tau → tau-jet + tau-neutrino) Tau-jet identification is important 27-May-2008 Stefan Stonjek: Missing Energy and Tau in ATLAS

Stefan Stonjek: Missing Energy and Tau in ATLAS What is ET,miss Not all energy originating from the hard interaction is measured in the detector E.g. neutrinos Sum of transverse Energy (ET) measured int the detector should be 0 Protons collide head on ET,miss = - SUM(ET)all visible particles Reconstruction of ET,miss is hampered by detector imperfection and wrong particle identification 27-May-2008 Stefan Stonjek: Missing Energy and Tau in ATLAS

ET,miss reconstruction algorithms Cell-based Only calorimeter cells which survive a noise suppression are counted Noise suppression Threshold based ( threshold = n × σ ; n=2 ) Topo cluster based (only use cells from topo clusters) Calorimeter cells above threshold “a” are used as seed cells Neighboring cell above threshold “b” are added to the cluster Border cells have to be above threshold “c” π0 – efficiency nearly 1 for 4/2/0 (> 4 GeV) ET,miss = ET,miss,calo + ET,miss,muon + ET,miss,cryo 27-May-2008 Stefan Stonjek: Missing Energy and Tau in ATLAS

Stefan Stonjek: Missing Energy and Tau in ATLAS Cell based ET,miss = ET,miss,calo + ET,miss,muon + ET,miss,cryo Calorimeter Separate energy calibration for Electromagnetic or hadronic showers H1-like or local-hadronic Muon Only muons with |η| < 2.7 (muon spectrometer geometry) For |η| < 2.5, muon spectrometer track matched with inner detector track Reduce fake muons Muon energy from muon spectrometer only (Avoid double counting) Cryostat Between LAr EM-calorimter and hadronic Tile-calorimeter ½ interaction length of uninstrumented material Jet energy has to be corrected 27-May-2008 Stefan Stonjek: Missing Energy and Tau in ATLAS

Refinement of Cell Based Topo clusters are assigned to reconstructed and identified objects Order: electron, photon, muon, had tau, b-jet, light jet Clusters belonging to two objects are assigned to first (above list) object If same class, energy is spread proportionally Cell calibration is adjusted accordingly Physics objects are better reconstructed Unassigned clusters are used as well with unassigned Topo clusters without 27-May-2008 Stefan Stonjek: Missing Energy and Tau in ATLAS

Stefan Stonjek: Missing Energy and Tau in ATLAS Object based Start with physics objects Distinguish between high (e/γ, μ, τ, jets) and low (π0, π±, unclustered) pT objects Mostly based on calorimeter Muons like in Cell-based Add calorimeter cells which are not related to high-pT physics objects Mini-jets are constructed from unassigned topo clusters (π± or π0 (if Ehad < 2% and PT > 10 GeV) ) Unassociated depositions are added to the ET calculation Performance of both methods are very similar Not specified which method was used for which plot 27-May-2008 Stefan Stonjek: Missing Energy and Tau in ATLAS

Resolution / Linearity Linearity = ET,miss,true – ET,miss,reco 27-May-2008 Stefan Stonjek: Missing Energy and Tau in ATLAS

Stefan Stonjek: Missing Energy and Tau in ATLAS Performance Z → tau + tau A → tau + tau mA = 450 GeV Tail due to non-Gausian effects caused by ET,miss mismeasurement 27-May-2008 Stefan Stonjek: Missing Energy and Tau in ATLAS

Stefan Stonjek: Missing Energy and Tau in ATLAS Fake ET,miss Muons Fake or missed high pT muon Calorimeter Cracks Leakage Instrumental defects E.g. calorimeter cells will fail Real data will provide a better calibration 27-May-2008 Stefan Stonjek: Missing Energy and Tau in ATLAS

Performance with Real Data Minimum bias events ET,miss,meas = 4.3 GeV (no beam gas or halo) Well known physics Calibrate ET,miss scale Z → leptop + lepton W → lepton + neutrino W / Z mass is well known 27-May-2008 Stefan Stonjek: Missing Energy and Tau in ATLAS

Stefan Stonjek: Missing Energy and Tau in ATLAS Tau decay Tau → muons/electron: 17.4%/17.8% (+ tau neutrino and muon/electron neutrino) Tau → hadrons: 64.8% (+ tau neutrino) One-prong: one charged pi π± + neutrino: 22.4% of one-prong π± + n π0 + neutrino: 73.5% of one-prong Three-prong: three charged pi 3π± + neutrino: 61.6% of three-prong 3π± + n π0 + neutrino: 33.7% of three-prong Only 0.1% five-prong to hard to detect in multi-jet environment 27-May-2008 Stefan Stonjek: Missing Energy and Tau in ATLAS

Tau reconstruction algorithms General idea Pencil like (very narrow) shaped jet, well collimated Difficult to quantify Leading track Two algorithms Calorimetry based Track-based Both calculate charge from tracks in core region Charge misidentification < 3.6% Tau production and decay well seperated in space and time Lifetime = 0.29 ps ; c × lifetime = 87.11 μm Secondary vertex identification seems possible (if more than one charged product) tau jet QCD jet 27-May-2008 Stefan Stonjek: Missing Energy and Tau in ATLAS

Calorimeter based algorithm Starting from calorimeter clusters the following variables are calculated Electromagnetic-Radius Isolation in the calorimeter Charge of candidate Number of associated tracks Number of hits in the η strip layer Transverse energy in the η strip layer Lifetime signed pseudo impact parameter significance ET over PT of the first track Likelihood of all of the above (1,2,4,5,6) Pencil-like, well collimated jet (7) 2-dim “secondary vertex” (three prong only) (8) leading track caries a large fraction of jet energy (one prong) 27-May-2008 Stefan Stonjek: Missing Energy and Tau in ATLAS

Stefan Stonjek: Missing Energy and Tau in ATLAS Track based algorithm Seeded by a good quality track (leading track) Combined with up to 6 tracks in core region (η,φ) and associated calorimeter information to form a candidate Energy flow approach Identification with calorimeter and tracking information Track Width of the tracks ; invariant mass of track system number of tracks in the isolation cone Calo Electromagnetic radius ; Number of strips ; width of deposit in the strips Faction of energy in outer ring 0.1 < ΔR < 0.2 ; isolation energy 0.2 < ΔR < 0.4 Track and calo Visible mass ; Visible mass from energy flow Energy in had-Cal relative to sum of track momenta Overall identification by cuts or MVA or Neural Net 27-May-2008 Stefan Stonjek: Missing Energy and Tau in ATLAS

Rejection rates / Efficiency Both algorithms work well Calo better for hight ET Track better for low ET About to be merged Calo likelihood Track Neural Network 27-May-2008 Stefan Stonjek: Missing Energy and Tau in ATLAS

Stefan Stonjek: Missing Energy and Tau in ATLAS Fake tau Main source of fake taus: QCD jets Fake rate: several per mile to several percent Much more QCD-jets than tau-jets For good measurements fake rate has to be determined 27-May-2008 Stefan Stonjek: Missing Energy and Tau in ATLAS

Collinear approximation Tau reconstruction is reconstruction of tau-jet Collinear approximation reconstruct tau from tau-jet and ET,miss Assumption ET,miss is sum of neutrino (tau → had) neutrino (tau → e/μ) Invariant mass of incoming particle can be calculated pencil-like jet tau neutrino tau incoming particle H / A / Z tau ET,miss tau neutrino μ 27-May-2008 Stefan Stonjek: Missing Energy and Tau in ATLAS

Stefan Stonjek: Missing Energy and Tau in ATLAS Summary and Outlook Tau events are a handle for new physics at LHC A good ET,miss reconstruction is important for tau analyses First data will improve ET,miss and tau reconstruction 27-May-2008 Stefan Stonjek: Missing Energy and Tau in ATLAS

Stefan Stonjek: Missing Energy and Tau in ATLAS The End 27-May-2008 Stefan Stonjek: Missing Energy and Tau in ATLAS

Stefan Stonjek: Missing Energy and Tau in ATLAS ET,miss and pile-up 27-May-2008 Stefan Stonjek: Missing Energy and Tau in ATLAS