Erik Devetak Oxford University SiD Workshop 24/02/2009

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Presentation transcript:

Erik Devetak Oxford University SiD Workshop 24/02/2009 t-tbar analysis at SiD Flavour tagging for ttbar Hadronic ttbar events ID Top Mass Charge Reconstruction t, b forward backward asymmetry Erik Devetak Oxford University SiD Workshop 24/02/2009 E. Devetak – Sid Benchmark

E. Devetak – Sid Benchmark Benchmarking LoI #5 AIM: in the all hadronic channel (e+e-→tt, t→bW, W→qq’) calculate: Top total cross – section Calculate mass of top quark Top forwards backwards asymmetry GOOD PROGRESS! First draft analysis! Clearly some algorithms need tuning/improvements! (we can do better everywhere) TOOLS: b tagging (LCFI) charge reconstruction (LCFI + ad hoc) Kinematic Fitting (MarlinKinfit) E. Devetak – Sid Benchmark

E. Devetak – Sid Benchmark The simulation process… Whizard - Pythia SLIC LOI Version OLD – Dev. Version Tracking FASTMC Marlin PFA Jet Clustering org.lcsim DATA PRESENTED: All SM, full reco Integrated L ≈ 458fb-1 One million top events used for “MC data” Flavour Tagging Analysis Marlin+ ROOT E. Devetak – Sid Benchmark

E. Devetak – Sid Benchmark TOOLS 1: Identifying the b quark Using LCFI Vertex package: Defaults tested on di-jet sample Need to check b tagging for 6 jets Originally developed by LCFI for LDC, check for Sid NN output b-tag for all SM events MC b-quark MC uds-quark MC c-quark Good Performance So far no parameter optimization for: SiD 6 jet sample Not envisaged in LOI timeframe Default on di-jet sample All SM events forced to 6jets, hence a lot of jet confusion! E. Devetak – Sid Benchmark

E. Devetak – Sid Benchmark t-t →bbqqqq Event Selection Perform jet clustering (force to 6 jets) Apply quality + background rejection cuts Sum of NN-btag of all six jets Number of particles in Event All Hadronic Top All Top All SM Total energy in Event After all other cuts Apply 6 simple cuts: No Isolated e/μ, Total Energy > 420 GeV , Number Particles > 80, Number Tracks > 30, -log(ycutmin) > -8, b-tagging cut. Still some cut optimization possible E. Devetak – Sid Benchmark 5

E. Devetak – Sid Benchmark Purity –Efficiency – Cross Section Started with 132454 hadronic events After Cuts 69708 remain Efficiency 52.6% Background Events 29605 Total Number of Events 99313 Purity 70.2% Note at present efficiency and backgrounds calculated from the same sample. In future calculate from separate sample (MC sample). This sample contains one million top events. Error on this should be small! Assume efficiency has no error. Cross section = (NEvents passing cut – NBG-Events passing cuts)/Efficiency Error = √(NEvents passing cut + NBG-Events passing cuts)/Efficiency Cross Section Error ≈ 845 events (or 360 measured events). Corresponds to 264.91+/-1.85 fb ( purely statistical error) Should be able to do better! Possible, do the same after Kinematic Fitting and apply mass cuts. E. Devetak – Sid Benchmark 6

E. Devetak – Sid Benchmark TOOLS 2: Kinematic Fitting Kinematic fitter performed after b tagging. 2 jets with highest b-tag treated a b jets others as jets from W. (and b mass assigned) Use hard constraints: #constraints Total energy 500GeV 1 Total momentum (x,y,z direction) =0 3 W1mass = W2mass = 80.4 2 top1mass = top2mass 1 Before fit (tops) After fit (events) After fit and cut (dashed Background) Top Mass Attempted also different constrains-combinatorics: Not use b tagging Not use W mass constrain Use only W1mass =W2mass Cut on probability event satisfies constrains (10% cut presented) E. Devetak – Sid Benchmark GeV

E. Devetak – Sid Benchmark Top Mass – Simple fitting, no prob. cut Function fitted: gauss (detector smearing) convoluted BW (intrinsic width) add tanh (best model found for additional background, empirical) from combinatorics! Purity: 91%, Efficiency: 43% Major issue is combinatorics background. Produces fat tails at high Mass! Some ideas … Results for 458fb-1: σm= 70MeV (statistical error) Peak displaced. Used 174.0GeV top at MC, fitting value 175.09 GeV. Issue understood tanh not good model. Reduce error from combinatorics. Lorentz half width > 5GeV. Calculate Cross Section error: 1.30 fb (better) E. Devetak – Sid Benchmark 8

E. Devetak – Sid Benchmark Top Mass – Simple fitting Apply 10% probability cut Purity: 94%, Efficiency: 19% Major issue is combinatorics background. Produces fat tails at high Mass! Much better fit (χ2/Dof ≈ 2.5), previously higher. (If cut only central region χ2/Dof < 2). Still same issues as before, but more under control. tanh not best function. Change! Results for 458fb-1: σm= 67MeV (statistical error) Peak displaced. Used 174.0GeV top at MC, fitting value 174.81 GeV. Issue understood tanh not good model. Seeking resolution. Lorentz half width > 8GeV. Not critical, understood, use double gaussian. Calculate Cross Section error: 1.96 fb (worse) E. Devetak – Sid Benchmark

E. Devetak – Sid Benchmark Top Mass Diversion – “template fitting” WITH ONLY ONE SAMPLE: Assume reconstruction and analysis differences minimal for Δm ≈ 1GeV Effectively assume infinite sample for MC template Take sample and shift it with steps of 0.5GeV Calculate χ2/dof Infer σmass of analysis Chi^2/dof vs. mass shift of top distribution Old Plot produced with fast MC Currently only experimented with FASTMC and no SM background PRELIMINARY RESULTS: Results with FastMC 50fb-1 show that result consistent with simple fitting Method does not suffer from combinatorics background problems! RESULT WILL BE USED FOR CONSISTENCY/SANITY CHECK E. Devetak – Sid Benchmark 10 10

E. Devetak – Sid Benchmark TOOLS 3: Charge Reconstruction Idea: develop series of discriminating variables, then recombining them Similar to what it is done in the flavour tagging. At present two charge reconstruction algorithms implemented (more can be added!): Momentum weighted secondary vertex charge - good for B+/B- if secondary found Momentum weighted Jet charge – Good for B0s and of no secondary. Variables chosen for ttbar hadronic! (different choices for different analysis?) Old Plot produced with fast MC Plot Produced with 1,000,000 top sample full reconstruction Purity vs. Efficiency B+/B- Combined M. Vertex Charge M. Jet Charge M. Vertex Charge M. Jet Charge E. Devetak – Sid Benchmark

E. Devetak – Sid Benchmark TOOLS 3: Combining charge variables To get Combined Charge variable: Use “MC data” to determine ratio of signal to backgrounds in each bin for each variable. Use this ratio as a discriminating power of each variable for that specific event. Multiplies the ratios of each variable considered. Apply transformation to get a result between -1 and 1. Combined charge b and bbar quarks Can use different assumptions of what is signal and what is background B+/B- (previous page) B0/B0 b/b (previous page) b quark bbar quark For asymmetry study: Use assumption b/b Multiply Combined Charge for 2 highest b-tag jets Cut: Combined Charge < -0.6 E. Devetak – Sid Benchmark NOTE: “granularity” from binning + “transformation” 458fb-1 top-topbar events passing cuts.

E. Devetak – Sid Benchmark t and b quark asymmetries Events used for b quark asymmetry b quark asymmetry Background 21% Total charge/flavour mis-tagging = 9% Asymmetry b quark: 0.29 +/- 0.02 Hence Purity 70%, Efficiency 5.9% Consistent with standard model input. At MC level 0.28 Events used for t quark asymmetry t quark asymmetry Same data as for b. Asymmetry t quark: 0.32+/- 0.02 At MC level 0.35 – consistent Need to recalculate error. Now using simple poisson error. (need binomial, no major change, can quote precision to next significant figure!) All reconstructed quarks Background (not ttbar event) Charge or flavour mistagged E. Devetak – Sid Benchmark

E. Devetak – Sid Benchmark Summary – Results (e+e-→tt, t→bW, W→qq’) All needed results available. If we were to finish this today we could quote: Cross section = 264.91+/- 1.30 fb Top Mass Error = 174.810+/- 0.067 GeV Afb b quark = 0.29 +/-0.02 (0.015) Afb t quark = 0.32 +/-0.02 (0.015) Given we have one month left: Use MC values from 1million top sample for efficiency calculation Deal with fat tail at high Mass of top mass and hence displaced peak Recalculate Template fitter for full reconstruction (no prob with displaced peak) Recalculate error on asymmetry (so we can quote 1 more sig. figure) Try to increase efficiency of Afb E. Devetak – Sid Benchmark