First Evidence for Electroweak Single Top Quark Production

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Presentation transcript:

First Evidence for Electroweak Single Top Quark Production XLIInd Rencontres de Moriond QCD and High Energy Hadronic Interactions La Thuile, 17-24th March 2007 First Evidence for Electroweak Single Top Quark Production Leonard Christofek on behalf of the D0 Collaboration Moriond 2007 Leonard Christofek, Brown University

Single Top Theory and Motivation s-channel (tb) t-channel (tqb) Associated production (tW) NLO = 0.88 ± 0.11 pb NLO = 1.98 ± 0.25 pb NLO ~ 0.21 pb Too small at Tevatron Study the Wtb coupling in top quark production measure |Vtb| directly (no assumption of 3 families) test unitarity of CKM matrix Cross section sensitive to new physics Background to SM Higgs production Test of techniques to extract small signal from dominant background Moriond 2007 Leonard Christofek, Brown University

Leonard Christofek, Brown University Window to new physics s-channel (tb) t-channel (tqb) Associated production c, W’, b, New heavy boson, New strong dynamics Flavor changing neutral currents (FCNC) Modified Wtb coupling Each new process would enhance single top quark production! Moriond 2007 Leonard Christofek, Brown University

Leonard Christofek, Brown University Event Signature High pT jet High pT lepton Missing transverse energy High pT jet (“b-tagged”) High pT jet (“b-tagged”) One isolated high transverse momentum lepton Missing transverse energy Two to four high transverse momentum jets One or two jets associated with b-quark: Labeled as a “b-tagged” jet Moriond 2007 Leonard Christofek, Brown University

Leonard Christofek, Brown University Backgrounds Top pair production normalized to NNLO cross section Multijet background modeled using data with a non-isolated lepton and jets W+jets (Wbb, Wcc, Wjj) and multijet background normalized to data before b-tagging Moriond 2007 Leonard Christofek, Brown University

Leonard Christofek, Brown University Analysis Strategy Binned Likelihood Cross Section or Limits Moriond 2007 Leonard Christofek, Brown University

Leonard Christofek, Brown University Background Model Source of Uncertainty Size Top pair normalization 18% W+jet & multijet norm. 18-28% Integrated luminosity 6% Trigger modeling 3-6% Lepton ID corrections 2-7% Other small components Few% Jet energy calibration 1-20% “b”-tagged jet modeling 2-16% Signal acceptances: tb=(3.2 ± 0.4)% tqb=(2.1 ± 0.3)% Single top signal smaller than total background uncertainty Cross section uncertainty dominated by statistical uncertainty Moriond 2007 Leonard Christofek, Brown University

Bayesian Neural Networks Use 24 variables for training networks (input nodes). Train network on signal and background simulated events: Signal tends to one and background tends towards zero (output node). Average many different networks for stability (hidden nodes). Less prone to over-training. Input Nodes Hidden Nodes Output Node tqb Wbb Moriond 2007 Leonard Christofek, Brown University

Leonard Christofek, Brown University Matrix Element Use full kinematical information contained in event (i.e. the four vectors from the lepton and jets). Compute the probability for that event configuration to occur. Backgrounds: Wbb, Wcg, Wgg, Wbbg Moriond 2007 Leonard Christofek, Brown University

Leonard Christofek, Brown University Decision Trees Goal: recover events that fail a simple cut-based analysis Use 49 variables for training: most discriminating variables M(alljets), M(W,b-tag1), cos(b-tag1,lepton), Q(lepton)*(untagged1) Decision tree output for each event = leaf purity: NS/(NS+NB) Train network on signal and background simulated events: Signal tends to one and background tends towards zero Boosting: retrain 20 times to improve “weak classifier” Moriond 2007 Leonard Christofek, Brown University

Expected and Observed Results Bayesian NN Matrix Element Decision Trees Exp. Obs. (tb+tqb)[pb] 3.2 +2.0-1.8 5.0 ± 1.9 3.0 +1.8-1.5 4.6 +1.8-1.5 2.7 +1.6-1.4 4.9 ± 1.4 Significance 1.3 2.4 1.8 2.9 2.1 3.4 First evidence for single top quark production! SM compatibility is 11%. Moriond 2007 Leonard Christofek, Brown University

Leonard Christofek, Brown University Discriminant Output Moriond 2007 Leonard Christofek, Brown University

Leonard Christofek, Brown University Extracting |Vtb| Assuming standard model production: Pure V-A and CP conserving interaction: f1R = f2L = f2R = 0. |Vtd|2 + |Vts|2 << |Vtb|2 or B(t Wb) ~ 100%. 0.68 < |Vtb| < 1 at 95%CL (f1L = 1) |Vtb f1L| = 1.3 ± 0.2 Moriond 2007 Leonard Christofek, Brown University

Leonard Christofek, Brown University Combination Highly correlated. Correlation matrix  = 4.8 ± 1.3 pb Significance = 3.5  Preliminary Moriond 2007 Leonard Christofek, Brown University

Leonard Christofek, Brown University Summary First evidence for single top quark production. With 3.5  significance. 4.8 ± 1.3 pb First direct measurement of | Vtb | Now starting to analyzing full 2 fb-1 data set. Onto observation! Moriond 2007 Leonard Christofek, Brown University

Backup Transparencies Moriond 2007 Leonard Christofek, Brown University

Leonard Christofek, Brown University Outline Theory and motivation for single top Event signature Backgrounds Multivariate analyses: Bayesian Neural Network, Matrix Elements, Decision Trees Cross section and signal significance Combination of measurements Measurement of the CKM element |Vtb| Summary Moriond 2007 Leonard Christofek, Brown University

Discriminating Variables Moriond 2007 Leonard Christofek, Brown University

Leonard Christofek, Brown University Single Top Monte Carlo Based on COMPHEP Reproduces NLO kinematic distributions PYTHIA for parton hadronization Moriond 2007 Leonard Christofek, Brown University

Systematic Uncertainties Full treatment of systematics. Each systematic is turned off and the cross section reevaluated. The contribution of each systematic is estimated by taking subtracting these two widths in quadrature. Moriond 2007 Leonard Christofek, Brown University