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Studies of Diboson Production and Triple Gauge Boson Couplings
7/27/2006 Studies of Diboson Production and Triple Gauge Boson Couplings Zhengguo Zhao University of Michigan, Ann Arbor, USA 9th ACFA Physics and Detector Workshop& ILC GDE Meeting Feb. 4-7, 2007, Beijing 1/5/2007 Beijing, Zhengguo Zhao
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Outline Introduction Recent Tevatron results Effort from ATLAS/CMS
7/27/2006 Outline Introduction Recent Tevatron results Effort from ATLAS/CMS Summary 1/5/2007 Beijing, Zhengguo Zhao
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Introduction 1/5/2007 Beijing, Zhengguo Zhao
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Diboson Production at Hadron Collider
V3 V1 V2 q q’ LO Feynman diagram, V1, V2, V3 = Z, W, g WW, ZW, ZZ, Wg. Production cross section predictable Only s channel has three boson vertex, which manifest the gauge boson coupling SM: Pure neutral vertexes ZZZ, ZZ g are forbidden (Z/g carry no charge and weak isospin that needed for gauge bosons couple) Only charged couplings WWg, WWZ are allowed 1/5/2007 Beijing, Zhengguo Zhao
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Triple Gauge Boson Couplings
Characterized by an effective Lagrangian, parameterized in terms of coupling parameters for new physics C, P and CP symmetry conservation, 5 free parameters: - lg ,lZ: grow with s, big advantage for LHC - kg = kg-1, g1Z = g1Z-1, kZ = kZ-1: grow with s Tree level SM: lg = lZ = kg = g1Z = kZ = 0 1/5/2007 Beijing, Zhengguo Zhao
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Production of WZ, WW q q’ W Z l+ l- l n l s-channel dominates,
Sensitive only to WWZ coupling Clean signal eee, eem, mme, mmm 3 isolated high pT leptons with large ET(miss) s-channel l Sensitive to WWZ and WWg Clean signal ee, mm, em 2 isolated high pT leptons with opposite charge and large missing ET s-channel t-channel 1/5/2007 Beijing, Zhengguo Zhao
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Production of Wg, ZZ Isolated high pT lepton (e, m) large missing ET
Isolated g Main bkg: W+jet, Z+ g s channel suppressed by O(10-4) Only t-channel at tree level, 4 isolated high pT leptons from the Z pair decays Clean signal eeee, eemm, mmmm, almost bkg free z l+ l- l’+ l’- q qbar q’ z 1/5/2007 Beijing, Zhengguo Zhao
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Diboson as background for searches
ZZ H 1/5/2007 Beijing, Zhengguo Zhao
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Motivations • Measure diboson production and TGCs
• Explore none-Abelian SU(2)U(1) gauge structure of SM • Probe new physics if production cross section, or TGCs deviate from SM prediction complementary to direct search for new physics • Understand the backgrounds of many important physics analyses Search for Higgs, SUSY, graviton and study of ttbar 1/5/2007 Beijing, Zhengguo Zhao
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Recent Results from Tevatron
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WW Production at Tevatron
L(pb-1) Nobs/Nb (pb) D0 25/9.8 CDF 825 95/43.4 13.6±2.3(stat) ±1.6(sys) ±0.9(lum) NLO 12±0.8 1/5/2007 Beijing, Zhengguo Zhao
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WW+WZlnjj 1 lepton with pT>25GeV, ET>25 GeV
≥2 jets with pT > 15 GeV (WW+WZ) < 36 95% CL 1/5/2007 Beijing, Zhengguo Zhao
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WW+WZlnjj anomalous coupling from CDF
Select 56 < mjj < 112 peak region Minimize likelihood for pT of W(l,ET) -0.51 < < 0.44, < l < 0.28 1/5/2007 Beijing, Zhengguo Zhao
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WZ lnll q q’ W Z l+ l- l n 3 leptons (e, m) - CDF: pT(leading) >20 GeV, pT(others) > 10 GeV - D0: pT(all) > 15 GeV m(l+l-) within mZ window ET is used to suppress the bkg of Z+jet/g 1/5/2007 Beijing, Zhengguo Zhao
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WZ lnll results L(pb-1) Nobs (pb) D0 760-860 12 7.5 ± 1.2 3.6 ± 0.2
CDF 825 2 3.7 ± 0.3 0.9 ± 0.2 < 6.3 (95% CL) NLO 3.7 ± 0.1 1/5/2007 Beijing, Zhengguo Zhao
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WWZ Anomalous Coupling
For L = 300 pb-1 data, expect 2 signal and 1 background events. Observed 3 events. TGCs are determined to be 1/5/2007 Beijing, Zhengguo Zhao
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(Wglng) from D0 Channel L(pb-1) (pb) Wgeng 933 3.12 ± 0.49 ± 0.19
Wgmng 878 3.21 ± 0.49 ± 0.2 SM 3.21±0.08 1/5/2007 Beijing, Zhengguo Zhao
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Tevatron Results on Dibson Studies
Tevatron results consistent with SM prediction 1/5/2007 Beijing, Zhengguo Zhao
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Diboson Studies from ATLAS and CMS
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LHC Expectations for the TGCs
High CM energy larger s High luminosity high statistics High sensitivity Expected to be ~10 improvement on LEP/Tevatron Predictions for TGCs at 95% C.L. for L=30 fb-1 (inc syst) < lg < < lZ < < Dkg < -0.11 < DkZ < +0.12 < Dg1Z < 1/5/2007 Beijing, Zhengguo Zhao
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MC Data for Diboson Studies(ATLAS)
7/27/2006 MC Data for Diboson Studies(ATLAS) Process MC data ZW+ 2e/2m + X 26033 ttbar l+x 1.96105 ZW- 2e/2m + X 29085 ee/mm/ tt 2.30106 ZZ 4e, 4m, 2e2m 19933 W e/m/t + n 1.61106 WW ln + x 32056 W+jets ln + x 1.59106 ZZ(pythia) 4 l (e,m) 4.66104 Z+jet ee/mm/tt 5.80106 Zbb4 l 4.99104 DY Z/g l+ l- (e, m, t) 1.67107 Zg ll (e,m) 2.50104 Data produced in ATLAS GRID, and Michigan ATLAS computer cluster Background (pythia 6.2), 106 ~ 107 for Z+jet, W+jet, DY, W+jet and Wlepton Signal events produced by (v2.3)–Jimmy, W/Z width effect is not included (v3.1 has included width) 1/5/2007 Beijing, Zhengguo Zhao
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ZW Signal and Backgrounds(ATLAS) (for 1 fb-1 data)
Neee Neem Nmme Nmmm Ntotal(1fb-1) Nsignal 16.9 17.1 21.9 19.8 75.7 Nbkg 1.71 0.88 1.73 2.00 6.32 S/B 9.84 19.4 12.7 9.92 12.0 47.4% 42.9% 7.7% 2.1% 1/5/2007 Beijing, Zhengguo Zhao
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WW Signal and Background (ATLAS) (for 1 fb-1 data)
Process Nee Nmm Nem Ntotal WWl+X (l=e,m) 36.7 37.6 284.4 358.7 Total background 188.6 112.1 59.4 360.1 S/B 0.19 0.34 4.79 1.0 47.3% 38.4% 8.3% 3.4% 2.6% 1/5/2007 Beijing, Zhengguo Zhao
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Invariant Mass and Pt Distributions for ZZ
For 1 fb-1 data at ATLAS M(e+e-) M(m+m-) Pt(e+e-) Pt(m+m-) 13 events candidates Background free with current statistics 1/5/2007 Beijing, Zhengguo Zhao
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Comparison of the efficiencies of BDT/ANN
Background efficiency Signal efficiency 1/5/2007 Beijing, Zhengguo Zhao
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Signal and Background Samples (CMS)
×Br k-factor ZZ(4e) 18.7 fb 1.3 WZ(3l, l=e,m,t) 1.6 pb 1.92 ttbar(2l) 62.3 pb 1.6 Z(ee)bb 60.3 pb 2.4 Z(mm)bb ttbar(4e) 194 fb ZZ(2e2m) 32.3 fb 1.35 Signal Main bkg tt(2l) generated with TopReX, Zbb with CompHEP, all others with Pythia 1/5/2007 Beijing, Zhengguo Zhao
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WZ→3l Expected Signal & Background
M(l+l-) after all cuts 4 channels combined (3e,2e1m,2m1e,3m) Presence of peaking backgrounds - Zbb - ZZ (irreducible) High significance in the first 1 fb-1 L = 1 fb-1 Expected signal and background yields for 1 fb-1 1/5/2007 Beijing, Zhengguo Zhao
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ZZ→4e Expected Signal & Background
L = 10 fb-1 M(e+e-) after all cuts (2 entries per event) Nearly background free! Expected signal and background yields for 1 and 10 fb-1 1/5/2007 Beijing, Zhengguo Zhao
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WZ and ZZ Discovery Potential (CMS)
ZZ→4e signal significance WZ →3l signal significance Ideal simulation miscalibration Systematic effects Ideal simulation miscalibration Systematic effects 5 s discovery ZZ: ~1 fb-1 WZ: ~150 pb-1 1/5/2007 Beijing, Zhengguo Zhao
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Summary D0 and CDF have been actively studies diboson production and the corresponding TGCs. The results so far are consistent with SM predictions. WZ, WW and ZZ signals are expected to be established at CMS and ATLAS with 100pb-1~1fb-1 Anonymous gauge boson coupling can be probed with a few fb-1 data Advanced techniques (BDT, ANN) can significantly improve the S/B. To improve the TGCs with LHC data, it’s crucial to correctly build the TGCs into event generators 1/5/2007 Beijing, Zhengguo Zhao
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Experiments at Tevatron
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CDF & D0 Detectors CDF Run II Upgrades:
New Silicon Vertex Detector (SVX) and faster tracking drift chamber (COT) New scinitllating-tile end-plug calorimeters Increased ηφ coverage for muon detectors New Scintillator Time-Of-Flight system D0 Run II Upgrades: New silicon (SMT) and Fiber (CFT) trackers, placed in new 2T Solenoid Calorimeters supplemented with Preshower detectors Significantly improved Muon System 1/5/2007 Beijing, Zhengguo Zhao
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1/5/2007 Beijing, Zhengguo Zhao
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The LHC Experiments 4.5 km 1/5/2007 Beijing, Zhengguo Zhao
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Collisions at the LHC 2804 bunch/beam 7 + 7 TeV
Particle Parton (quark, gluon) Proton l jet Bunch SUSY..... Higgs Z o e + - 2804 bunch/beam 7 + 7 TeV separation: 7.5 m (25 ns) 40 MHz crossing rate 1011 proton / bunch 109 pp collision/s (superposition of 23 pp interactions per bunch crossing: pile-up) N = L × (pp) = 109 Mostly low pt events (soft) events Interesting high pt events are rare New physics rate ~ Hz event selection: 1 in 10,000,000,000,000 1/5/2007 Beijing, Zhengguo Zhao
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Length: ~ 46 m Radius : ~ 12 m Weight : ~ 7000 tons Channels: ~ 108
7/27/2006 Muon spectrometer air-core toroids, MDT+RPC+TGC s/pT ~ 2-7 % |h| < 2.7, |h|<2.5 ( precision phys.) Length: ~ 46 m Radius : ~ 12 m Weight : ~ 7000 tons Channels: ~ 108 Lcable: ~ 3000 km EM Calorimetry Pb-LAr s/E ~ 10%/√E(GeV)1% |h|<3.2, |h| < 2.5 (fine granularity) a Inner detector Si pixels and strips Transition Radiation Detector (e/ separation) s/pT ~ 0.05% pT(GeV)0.1%; |h| < 2.5, B=2 T(central solenoid) Hadron Calorimeter Fe/scintillator (central), Cu/W-LAr (fwd) s/E ~ 50%/√E(GeV)3% ||<3 1/5/2007 Beijing, Zhengguo Zhao
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Silicon pixels and strips
EM calorimeter: Lead tungstate s/E = 5% / √E (GeV) 2% Muon spectrometer DT+CSA+RPC Magnet solenoid 4 T Hadron Calorimeters Barrel & Endcap: Cu/Scintillating sheets s/E = 65% /√E (GeV)5% Inner Detector: Silicon pixels and strips 1/5/2007 Beijing, Zhengguo Zhao
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Anomalous Coupling and Form Factor
Cross section increase for coupling with non-SM values, yielding large cross section at high energies that violating tree level unitarity form factor scale s: subprocess CM energy. L: form factor scale TGCs manifest in - cross section enhancement - high pT(V=Z,W,) - production angle 1/5/2007 Beijing, Zhengguo Zhao
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Diboson Production Cross Section
Tevatron LHC 1/5/2007 Beijing, Zhengguo Zhao
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Boosted Decision Trees (BDT) and Artificial Neural Network (ANN)
ATLAS e-boost ANN 1/5/2007 Beijing, Zhengguo Zhao
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WZ tt MZ(ee) Vector∑Et(jet) MZ(mm)-MW(en) cut Pt(l+l-) WW ZZ Zjet Zg
Pt(l+l-) cut to reject fate events Vector∑Et(jet) tt to reject jet MZ(ee) MZ(mm)-MW(en) WZ 1/5/2007 Beijing, Zhengguo Zhao
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