Update on Search for Resonant Slepton Production
|
|
- Jason Flynn
- 6 years ago
- Views:
Transcription
1 Overview Update on Search for Resonant Slepton Production Christian Autermann III. Phys. Inst. A, RWTH Aachen Luminosity Di-µ Trigger Efficiency & Error QCD Estimation New Limits Supported by Christian Autermann New Phenomena Meeting, / 2
2 Luminosity Question: Why was the luminosity 347 pb -? I was not yet using the v3 data. Now: good recorded Luminosity: ± 24.5 pb - Now using all data until shutdown 24 Removed 2.76 bad runs Removed bad LBNs. Christian Autermann New Phenomena Meeting, / 2
3 2µ-Trigger Efficiency Question: Why is the trigger eff. error so large? Di-muon Trigger Efficiency ε trigger = 94 ± 6 % correction factor.8.6 mean.939 ± di-µ trigger eff. ± σ syst. error stat. uncertainty η µ 2 Christian Autermann New Phenomena Meeting, / 2
4 2µ Trigger Efficiency (top_trigger) η-dependency of L (muptxatxx) and L2 is parameterized by: f 2 A ( η A2 ) 2 ( η) = A + A e sin( η A ) 3 2 with the parameters: A A A 2 A 3 Level : muptxatxx 2-4 ± ±.3 3.2±.2.998±.5 Level 2: MUON(,med) -.3±.6.±.9 See the top group s Note 452 for detail! -.7±.9.98±.2 from latest top_trigger release Trigger uncertainty of σ is defined by the uncertainty of these parameters. (top_trigger methods set_sigma & EventWeight) Christian Autermann New Phenomena Meeting, / 2
5 MC weight (trigger efficiency) weight.9 2µ Trigger η-parameterisation MU trigger turnon L3 + max. error L3 + σ LL2L3 Total L3 - σ L3 - max error trigger efficiency all parameter errors chosen randomly inside their range maximal error (error propagation) this is what top_trigger does η Christian Autermann New Phenomena Meeting, / 2
6 Error on Trigger Efficiency Ok, the error of the trigger efficiency is (too) large: 94 ± 6 % The reason is probably, that σ deviation is not given by the maximal variation of the parameters inside their errors But the systematic error of the trigger efficiency on preselection with 2 jets is only: 4. % The trigger error is negligible to other errors: (JES:.5%, QCD 6.6%, Lumi 6.5%) Even though it is estimated very conservatively Christian Autermann New Phenomena Meeting, / 2
7 QCD Estimation Question: Why did the QCD events peak at the Z-resonance? Redid the QCD estimation, now: almost same isolation cuts on data/signal and QCD more statistics QCD Criteria: b-tag one of both muons must NOT be isolated with respect to - Σ E T in hollow cone R=.4, r=. OR - Σ p_ T (track) in cone R=.5 number of events /. GeV Reconstructed Z-mass DO RunII preliminary Data Signal, point #58 QCD from Data tt->ll tt->l+jet Y Y s 2 s WW->µνµν WZ incl. ZZ incl. 5-5GeV 5-6GeV 4 5-6GeV 5 6-3GeV 4 6-3GeV GeV 25-5GeV 5-GeV 5-6GeV 5 6-3GeV 4 6-3GeV GeV 25-5GeV 5-GeV inv. di-muon mass [GeV] Christian Autermann New Phenomena Meeting, / 2
8 In the last talk, not enough points were processed. The limit was increasing with the slepton mass, because the inter/extrapolation failed. [GeV] m /2 Now I have enough points (275), (at least for tan(β)=5, sign(µ)=-) Limits τ tan(β)=5, sign(µ)=- is the LSP D RunII preliminary χ = GeV χ =75 GeV λ Not allowed l=2 GeV l=3 GeV 95% CL Exclusion Contour Gen. points excl. (λ 2 =.7) Gen. points (not excluded) [GeV] m Christian Autermann New Phenomena Meeting, / 2
9 Limit vs. Neutralino mass Fixed parameters: A =, sign(µ)=, tan β = 5, λ 2 =.7 Slepton mass = 2 GeV Slepton mass = 3 GeV limit,σ [pb] 3 25 λ 2 =.8 D RunII preliminary σ tot, l=2gev, tan(β)=5 Limit 95% CL limit,σ [pb] 8 7 λ 2 =.9 D RunII preliminary σ tot, l=3gev, tan(β)=5 Limit 95% CL 6 2 λ 2 =.7 5 λ 2 = λ 2 =.6 λ 2 =.5 λ 2 =.4 λ 2 =.3 Excluded Not allowed Neutralino mass χ [GeV] λ 2 =.7 λ 2 =.6 λ 2 =.5 λ 2 =.4 λ 2 =.3 Excluded Not allowed Neutralino mass χ [GeV] Christian Autermann New Phenomena Meeting, / 2
10 Limit vs. Slepton mass Fixed parameters: A =, sign(µ)=, tan β = 5, λ 2 =.7 Neutralino mass = 75 GeV Neutralino mass = GeV limit,σ [pb] D RunII preliminary σ tot, χ =75GeV, tan(β)=5 Limit 95% CL limit,σ [pb] 4 2 D RunII preliminary λ 2 =.8 σ tot, χ =GeV, tan(β)=5 λ 2 =.7 Limit 95% CL Not allowed λ 2 =.3 λ 2 =.7 λ 2 = Not allowed λ 2 =.5 λ 2 =.4 λ 2 =.3 5 Excluded Slepton mass l [GeV] 2 Excluded Slepton mass l [GeV] Christian Autermann New Phenomena Meeting, / 2
11 More limits (in progress ) [GeV] m /2 tan(β)=5, sign(µ)= τ is the LSP D RunII preliminary χ = GeV.4 λ χ =75 GeV.4 [GeV] m / tan(β)=5, sign(µ)=+ τ is the LSP l=2 GeV D RunII preliminary l=3 GeV χ = GeV χ =75 GeV 95% CL Exclusion Contour 5 Gen. points excl. (λ 2 =.7) Not allowed Gen. points (not excluded) m [GeV] λ 2 λ 95% CL Exclusion Contour 5 Gen. points excl. (λ 2 =.7) Not allowed Gen. points (not excluded) m [GeV] D RunII preliminary Christian Autermann New Phenomena Meeting, / 2 [GeV] m /2 tan(β)=5, sign(µ)= τ is the LSP l=2 GeV l=2 GeV l=3 GeV l=3 GeV χ = GeV χ =75 GeV 95% CL Exclusion Contour 5 Gen. points excl. (λ 2 =.7) Not allowed Gen. points (not excluded) [GeV] m λ
12 To Do Update note with limits for tan(β)=5, sign(µ)=+, tan(β)=5, sign(µ)=-, tan(β)=5, sign(µ)=+ Give limits more independent with respect to SUSY parameters (any suggestions welcome) Christian Autermann New Phenomena Meeting, / 2
13 Old Talk Christian Autermann New Phenomena Meeting, / 2
14 Overview Search for Resonant Slepton Production Christian Autermann III. Phys. Inst. A, RWTH Aachen Event Topology Data Selection and Efficiencies Control Plots Preliminary Exclusion Limits Outlook Supported by Christian Autermann New Phenomena Meeting, / 2
15 R-parity Violating Supersymmetry R - parity : W W R/ P = = W 2 MSSM ijk R P + i = ( ) W j R/ P k 3B+ L+ 2S ' λ L L E + λ L Q D + ijk i S is the particle spin, B is the baryon number, L is the lepton number j k '' λ ijk U i D j D k R-parity violating extension of the MSSM i,j,k =,2,3 generation indices R-parity conserving production associated/pair production of gauginos decay via λ ijk into 4 charged leptons require 3 charged leptons for analysis e e + X : Anne-Marie Magnan (λ 2 ) µ µ + X : Daniela Käfer (λ 22 ) τ + X : Anne-Catherine Le-Bihan (λ 33 ) Resonant production via λ 2 of smuon or sneutrino Cascade decay to LSP (neutralino) decay via λ 2 into 2 jets & lepton Chiral superfields: L: lepton doublet superfield E: lepton singlet superfield Q: quark doublet superfield D: down-like quark singlet superfield λ, λ`, λ``: Yukawa couplings Christian Autermann New Phenomena Meeting, / 2
16 Slepton Decay Channels Final State consists of 2 jets and up to two muons or missing E T Huge background from multi-jet processes Need to select events with at least 2 muons u u d µ µ d ν µ u 2 Muon Channels: Golden channel if l is a muon No ν, no missing E T Possible to reconstruct the neutralino and the slepton mass But only 25% branching ratio Other channels with MET and a second muon from cascade processes Not possible to reconstruct the slepton mass and not necessarily the neutralino mass. But higher branching ratio Christian Autermann New Phenomena Meeting, / 2
17 Signal Branching Ratios no muon one muon two muons ( golden channel ) Christian Autermann New Phenomena Meeting, / 2
18 Data Sample & Preselection Data from April 22 August 24 good recorded Luminosity: 347 pb - (preliminary) Preselection Sample Any Dimuon trigger has fired Veto against cosmic muons (Scintillator timings) 2 good muons with pt > 2 GeV, pt > 8 GeV central track match & isolation for both muons events, expected background: 2 984±67(stat)±54(syst) event Corrected for - Dimuon Trigger efficiency - Muon reconstruction efficiencies - Isolation efficiencies - Track finding & matching - Muon momentum smearing - Jet energy scale - Monte Carlo LO NNLO cross section Christian Autermann New Phenomena Meeting, / 2
19 Data Consistency: Preselection () number of events /.8 GeV Reconstructed Z-mass Statistics Data Signal, point # QCD from Data inv. di-muon mass [GeV] tt->ll tt->l+jet Y Y s 2 s WW->µνµν WZ incl. ZZ incl. 5-5GeV 5-6GeV 4 5-6GeV 5 6-3GeV 4 6-3GeV GeV 25-5GeV 5-GeV 5-6GeV 5 6-3GeV 4 6-3GeV GeV 25-5GeV 5-GeV Dominant SM MC is Z/γ µµ QCD is estimated from Data by a) using data events with like-sign, nearly isolated muons b) data events with b-tag Best agreement with method (b). Signal x (m χ =9GeV, m µ =263GeV) Other considered but negligible SM backgrounds: ttbar ll, ttbar l jet Z ττ Y(s), Y(2s) W µν ZZ, WZ, WW Christian Autermann New Phenomena Meeting, / 2
20 Data Consistency: Preselection (2) Preselection & jet p T > 5 GeV Transverse Momentum of jet Transverse Momentum of jet number of events /.5 GeV data Statistics Data Signal, point # QCD from Data signal x tt->ll tt->l+jet 5-5GeV Z/γ GeV 4 5-6GeV 5 6-3GeV 4 Z/γ 5-6 GeV Z/γ ->µµ 6-3GeV GeV 25-5GeV Z/γ ->µµ 5-GeV QCD, b-tag data 5-6GeV 5 tt ll 6-3GeV 4 6-3GeV GeV 25-5GeV 5-GeV jet p T [GeV] Ys 2 Ys WW->µνµν WZ incl. ZZ incl. number of events /.5 GeV data signal x Statistics Data Signal, point #56 SM ± syst. ± stat. sytematic uncertainty jet p T [GeV] Signal x (m χ =9GeV, m µ =263GeV) Christian Autermann New Phenomena Meeting, / 2
21 Data Consistency: Preselection (3) number of events / 8. GeV Preselection & jet p T > 5 GeV & jet 2 p T > 5 GeV Reconstructed χ nd Mass with 2 data signal x Statistics Data Signal, point # QCD from Data inv. mass of µ 2, jet, jet 2 [GeV] tt->ll tt->l+jet Z/γ ->µµ 5-6GeV 4 Z/γ GeV 5 6-3GeV 4 Z/γ ->µµ 6-3GeV GeV Ys 2 Ys WW->µνµν WZ incl. ZZ incl. 25-5GeV 5-GeV 6-3GeV 4 6-3GeV GeV 25-5GeV 5-GeV µ Z/γ 5-6 GeV QCD tt ll number of events / 8. GeV Reconstructed χ Mass with st µ Statistics Data Signal, point #56 SM ± syst. ± stat. data signal x sytematic uncertainty inv. mass of µ 2, jet, jet 2 [GeV] Signal unscaled (m χ =9GeV, m µ =263GeV) Christian Autermann New Phenomena Meeting, / 2
22 Constant Corrections () MC eff. Data eff. correction Muon Reconstruction.938±..93±.2.973±.27 MURECOEFF skim, Z/DY6-3 Muon central track finding & matching.972±..988±..6±.6 2MU skim, Z/DY6-3 Muon track isolation.956±..944±.2.989±. 2MU skim, Z/DY6-3 Medium Muon.956±..97±..6±.6 2MU skim, Z/DY6-3 All Pass 2 Data Method: Tag & Probe Data eff. / MC eff. is flat for p T, η, φ and inv. µ-mass Christian Autermann New Phenomena Meeting, / 2
23 Constant Corrections (2) reconstruction isolation track matching η µ reco correction.8.6 mean.973 ±.27 µ isolation correction.8.6 mean.989 ±. µ track correction.8.6 mean.27 ±.27 φ p T µ reco correction µ reco correction mean.973 ±.27 murecoeff Data / Z/γ (6-3 GeV) mean.973 ±.27 murecoeff Data / Z/γ (6-3 GeV) φ.4 η µ isolation correction MU Data / Z/γ (6-3 GeV) µ isolation correction mean.989 ±. 2MU Data / Z/γ (6-3 GeV) φ η mean.989 ±. µ track correction µ track correction mean.29 ±.29 2MU Data / Z/γ (6-3 GeV) MU Data / Z/γ (6-3 GeV) φ η mean.29 ± murecoeff Data / Z/γ (6-3 GeV) 2MU Data / Z/γ (6-3 GeV) 2MU Data / Z/γ (6-3 GeV) p T [GeV] p T [GeV] p T [GeV] Christian Autermann New Phenomena Meeting, / 2
24 Other Corrections Data eff. MC correction factor 2µ Trigger (top_dq) 92.8 ± 6.8 % f( p T, η, φ, jet, ME T ) Jet energy scale jet jet jet jet jet jet f(p T,η,φ, ME T ) f(p T,η,φ, ME T, ) Muon p T smearing NNLO MC x-sec. corr. f(p T muon ) f( inv. µ mass ) Corrections depend on event kinematics, like p T, η, φ, MET Systematic uncertainties are derived by varying corrections by ± σ. Total muon efficiency: 8 ± 5 % Christian Autermann New Phenomena Meeting, / 2
25 2D Cuts Final selection Final signal selection on Preselection & with di-jets: slepton neutralino mass plane channel separation several other 2D cuts in planes with -di-µ mass - missing E T - R(µ µ 2 ) -µ p T +µ p T - inv. di-jet mass - sum of jet p T - R(jet jet 2 ) Each 2D cut is done when the signal efficiency purity is larger than a certain limit. [GeV] inv. mass of µ 2, jet, jet 2 Reconstructed Slepton & Neutralino Mass inv. mass of µ, µ 2, jet, jet 2 [GeV] Christian Autermann New Phenomena Meeting, / 2 5 Statistics Data Signal, point # QCD from Data Signal (mχ=9gev, mµ=263gev) channel with MET High signal purity can be achieved Strong dependence on msugra point Optimize all cut parameters for each 2D cut and each msugra point tt->ll tt->l+jet 5-6GeV 4 5-6GeV 5 6-3GeV 4 6-3GeV GeV 25-5GeV 5-GeV 6-3GeV 4 6-3GeV GeV 25-5GeV 5-GeV Ys 2 Ys WW->µνµν WZ incl. ZZ incl. golden channel
26 Data Consistency (3) Cut Flow An exemplary cutflow for the SUSY point m =2 GeV, m /2 =243 GeV: Jet cuts 2D cuts Christian Autermann New Phenomena Meeting, / 2
27 Preliminary Results msugra points ready analyzed ( tan β = 5, µ/ µ = - ) 49 points reconstructed 27 generated Scans for tan β = 5 and 2.5M signal events positive µ in progress Christian Autermann New Phenomena Meeting, / 2
28 Exclusion Contours A =, tanβ=5, sign(µ)= [GeV] m / τ is the LSP D RunII preliminary DØ RunII preliminary l=2 GeV l=3 GeV χ = GeV χ =65 GeV 95% CL Exclusion Contour 5 Gen. points excl. (λ 2 =.7) Not allowed Gen. points (not excluded) [GeV] m.4 λ mass [GeV] l DØ RunII preliminary Not allowed 95% CL Exclusion Contour Gen. points excl. (λ 2 =.7) Gen. points (not excluded) χ mass [GeV].4 λ m m /2 plane slepton neutralino mass plane Christian Autermann New Phenomena Meeting, / 2
29 Limit vs. neutralino mass Fixed parameters: A =, sign(µ)=, tan β = 5, λ 2 =.7 Slepton mass = 2 GeV Slepton mass = 3 GeV limit,σ [pb] 3 25 λ 2 =.8 D RunII preliminary σ tot, l=2gev, tan(β)=5 σ ( l χ +l), λ =.7 2 Limit 95% CL limit,σ [pb] λ 2 =.9 D RunII preliminary σ tot, l=3gev, tan(β)=5 σ ( l χ +l), λ =.7 2 Limit 95% CL 2 λ 2 =.7 5 λ 2 = λ 2 =.6 λ 2 =.5 λ 2 =.4 λ 2 =.3 Excluded Not allowed Neutralino mass χ [GeV] λ 2 =.7 λ 2 =.6 λ 2 =.5 λ 2 =.4 λ 2 =.3 Excluded Not allowed Neutralino mass χ [GeV] Christian Autermann New Phenomena Meeting, / 2
30 Limit vs. slepton mass Fixed parameters: A =, sign(µ)=, tan β = 5, λ 2 =.7 Neutralino mass = 65 GeV Neutralino mass = GeV limit,σ [pb] 3 25 D RunII preliminary σ tot, χ =65GeV, tan(β)=5 σ ( l χ +l), λ =.7 2 Limit 95% CL limit,σ [pb] 4 2 D RunII preliminary λ 2 =.8 σ tot, χ =GeV, tan(β)=5 λ 2 =.7 l χ σ ( +l), λ 2 =.7 Limit 95% CL Not allowed λ 2 =.4 λ 2 =.3 2 =.8 λ =.7 λ 2 Excluded Slepton mass l [GeV] Not allowed λ 2 =.5 λ 2 =.4 λ 2 =.3 Excluded Slepton mass l [GeV] Christian Autermann New Phenomena Meeting, / 2
31 Conclusions Search for RPV SUSY through the LQD coupling λ 2 2 muon preselection sample is well described by SM incl. QCD All efficiencies and systematic errors measured Efficient 2D final selection cuts Improved limits compared to DØ Run I Continuously generating more signal points: Publish Results Christian Autermann New Phenomena Meeting, / 2
Search for Resonant Slepton Production with DØ
Overview Search for Resonant Slepton Production with DØ Christian Autermann, III. Phys. Inst. A, RWTH Aachen Event Topology Data Selection and Efficiencies Control Plots Selection Optimization Preliminary
More informationSearch for Resonant Slepton Production with the DØ-Experiment
Overview Search for Resonant Slepton Production with the DØ-Experiment Christian Autermann, III. Phys. Inst. A R-parity violating Supersymmetry Resonant Slepton Production and Neutralino Decay Data selection
More informationSearch for R-parity violating Supersymmetry. III Phys. Inst. A, RWTH Aachen
R-parity violating Supersymmetry III Phys. Inst. A, RWTH Aachen Introduction to R-parity violating SUSY Three DØ searches via non-zero LLE (short and long lived LSP) and LQD couplings Perspectives for
More informationResonant Slepton Production
Overvew III. Physkalsches Insttut A Resonant Slepton Producton Chrstan Autermann III. Phys. Inst. A, RWTH Aachen The Sgnal Processes Lmt Calculaton Model-Independent Lmts Combned Lmts Supported by Chrstan
More informationSearch for Charginos and Neutralinos with the DØ Detector
SUSY 006, 06/3/006 Marc Hohlfeld Search for Charginos and Neutralinos with the DØ Detector Marc Hohlfeld Laboratoire de l Accélérateur Linéaire, Orsay on behalf of the DØ Collaboration SUSY 006, 06/3/006
More informationCMS Searches for New Physics
CMS Searches for New Physics Christian Autermann, for the CMS collaboration I. Phys. Inst. RWTH Aachen University, Germany QCD14 2 Overview Searches for New Physics at CMS Inclusive search for Supersymmetry
More informationSUSY Search Strategies at Atlas and CMS
1 SUSY Search Strategies at Atlas and CMS (Universität Hamburg) for the Atlas and CMS Collaborations All-hadronic SUSY search Leptonic Inclusive SUSY search Reach in the msugra plane supported by: SUSY
More informationEarly SUSY Searches in Events with Leptons with the ATLAS-Detector
Early SUSY Searches in Events with Leptons with the ATLAS-Detector Timo Müller Johannes Gutenberg-Universität Mainz 2010-29-09 EMG Annual Retreat 2010 Timo Müller (Universität Mainz) Early SUSY Searches
More informationSearch for Supersymmetry with the CMS - Detector
Search for Supersymmetry with the CMS - Detector Aachen 3a SUSY Group: Markus Merschmeyer, Arnd Meyer, Prof. Thomas Hebbeker, Holger Pieta, Daniel Teyssier 29. August 2007 Supersymmetry SUSY at CMS Computing,
More informationSUSY Phenomenology & Experimental searches
SUSY Phenomenology & Experimental searches Alex Tapper Slides available at: http://www.hep.ph.ic.ac.uk/tapper/lecture.html Reminder Supersymmetry is a theory which postulates a new symmetry between fermions
More informationMeasurement of the Z ττ cross-section in the semileptonic channel in pp collisions at s = 7 TeV with the ATLAS detector
Measurement of the Z ττ cross-section in the semileptonic channel in pp collisions at s = 7 TeV with the ATLAS detector Sofia Consonni Università di Milano & INFN XCVII Congresso Nazionale della Società
More informationHiggs and Z τ + τ in CMS
Higgs and Z τ + τ in CMS Christian Veelken for the CMS Collaboration Moriond EWK Conference, March 14 th 2011 Z τ + τ - Production @ 7 TeV τ + Z τ - CMS Measurement of Z/γ* l + l -, l = e/µ: σ BR(Z/γ*
More information14th Lomonosov Conference on Elementary Particle Physics Moscow, 24 August 2009
M. Biglietti University of Rome Sapienza & INFN On behalf of the ATLAS Collaboration 1 14th Lomonosov Conference on Elementary Particle Physics Moscow, 24 August 2009 Theoretically favored candidates for
More informationTop Quark Physics at the LHC
Top Quark Physics at the LHC Ayana Arce HEP 0 Lectures #7 March 4, 203 Outline Introduction 2 Why are top quarks interesting? 3 Creating Top Quarks 4 Identifying Top Quarks 5 Some LHC results 6 Beyond
More informationHIGGS Bosons at the LHC
ATLAS HIGGS Bosons at the LHC Standard Model Higgs Boson - Search for a light Higgs at the LHC - Vector boson fusion - Comparison to the Tevatron potential Measurement of Higgs boson parameters The MSSM
More informationSearches for New Phenomena with Lepton Final States at the Tevatron
Searches for New Phenomena with Lepton Final States at the Tevatron including charginos, neutralinos,, excited leptons and unexpected signatures Todd Adams Florida State University for the CDF and DØ Collaborations
More informationWZ di-boson production at CMS
WZ di-boson production at CMS 1 Outline Physics motivations Existing results (Tevatron s = 1.96TeV) Existing prospects for CMS at s = 14TeV Preliminary prospects for CMS at s = 7TeV 2 WZ Physics motivation
More informationThe Tevatron s Search for High Mass Higgs Bosons
The Tevatron s Search for High Mass Higgs Bosons Konstantinos A. Petridis University of Manchester On behalf of the CDF and DØ Collaborations K.A. Petridis (University of Manchester) Tevatron High Mass
More informationSearching for Supersymmetry at the LHC David Stuart, University of California, Santa Barbara. CMS SUSY Search, D. Stuart, June 2011, Lisbon!
Searching for Supersymmetry at the LHC David Stuart, University of California, Santa Barbara CMS SUSY Search, D. Stuart, June 2011, Lisbon! 1! Searching for Supersymmetry at the LHC David Stuart, University
More informationInclusive top pair production at Tevatron and LHC in electron/muon final states
Inclusive top pair production at Tevatron and LHC in electron/muon final states Andreas Jung for the ATLAS, CDF, CMS and D Collaboration Fermilab, DAB5 - MS 357, P.O. Box 5, Batavia, IL, 651, USA DOI:
More informationarxiv:hep-ex/ v1 15 Jun 2006
arxiv:hep-ex/6636v 5 Jun 6 SEARCHES FOR NEW PHYSICS IN LEPTON FINAL STATES CATALIN I. CIOBANU FOR THE CDF AND DØ COLLABORATIONS Department of Physics, University of Illinois at Urbana-Champaign, W. Green
More informationATLAS Discovery Potential of the Standard Model Higgs Boson
ATLAS Discovery Potential of the Standard Model Higgs Boson Christian Weiser University of Freiburg (on behalf of the ATLAS Collaboration) 14th Lomonosov Conference on Elementary Particle Physics Moscow,
More informationPhysics with Tau Lepton Final States in ATLAS. Felix Friedrich on behalf of the ATLAS Collaboration
Physics with Tau Lepton Final States in ATLAS on behalf of the ATLAS Collaboration HEP 2012, Valparaiso (Chile), 06.01.2012 The Tau Lepton m τ = 1.8 GeV, heaviest lepton cτ = 87 μm, short lifetime hadronic
More informationElectroweak Physics at the Tevatron
Electroweak Physics at the Tevatron Adam Lyon / Fermilab for the DØ and CDF collaborations 15 th Topical Conference on Hadron Collider Physics June 2004 Outline Importance Methodology Single Boson Measurements
More informationSearches for Supersymmetry at ATLAS
Searches for Supersymmetry at ATLAS Renaud Brunelière Uni. Freiburg On behalf of the ATLAS Collaboration pp b b X candidate 2 b-tagged jets pt 52 GeV and 96 GeV E T 205 GeV, M CT (bb) 20 GeV Searches for
More informationCMS. Saeid Paktinat. On behalf of the CMS Collaborations. (IPM, Tehran)
SUSY @ CMS (IPM, Tehran) On behalf of the CMS Collaborations outline SUSY Common Signatures Some Examples Conclusion 2 Why SUperSYmmetry(1) SM describes a lot of experimental results very precisely, but
More informationFirst studies towards top-quark pair. dilepton channel at s = 13 TeV with the CMS detector
First studies towards topquark pair differential cross section measurement in the dilepton channel at s = 13 TeV with the CMS detector Mykola Savitskyi, Maria Aldaya, Carmen Diez Pardos et al. DESYCMS
More informationPDF Studies at LHCb! Simone Bifani. On behalf of the LHCb collaboration. University of Birmingham (UK)
PDF Studies at LHCb! Simone Bifani University of Birmingham (UK) On behalf of the LHCb collaboration MENU 213 Rome 3th September - 4th October 213 Outline Introduction Analyses» Z/γ* ll, l =, e, τ#» W
More informationHiggs Searches at CMS
Higgs Searches at CMS Ashok Kumar Department of Physics and Astrophysics University of Delhi 110007 Delhi, India 1 Introduction A search for the Higgs boson in the Standard Model (SM) and the Beyond Standard
More informationTop and Electroweak Physics at. the Tevatron
Top and Electroweak Physics at 1 the Tevatron Graham W. Wilson University of Kansas for the CDF and DØ Collaborations April APS 2008, St. Louis, MO. April 12 th 2008 Introduction Top Physics Overview Cross-section
More informationICHEP 2008 Philadelphia
ICHEP 2008 Philadelphia LHC CERN Geneva 2008 Sascha Caron Standard SUSY at LHC 2 Almost all LHC sectors are cooled down (2 sectors at this moment at 20-30K) Start at s = 10 TeV in 2008 2008 Luminosity
More informationSearch for Pair Production of Stop Quarks Mimicking Top Event Signatures
CDF/PUB/TOP/PUBLIC/9343 Search for Pair Production of Stop Quarks Mimicking Top Event Signatures The CDF Collaboration URL http://www-cdf.fnal.gov May 29, 2008 Abstract We present the search for the pair-produced
More informationCarlos Sandoval Universidad Antonio Nariño On behalf of the ATLAS collaboration DIS Kobe, Japan
Carlos Sandoval Universidad Antonio Nariño On behalf of the ATLAS collaboration DIS 2018 - Kobe, Japan 1 Search for long-lived massive particles (LLP) in events with displaced vertices (DV): arxiv:1710.04901v1
More informationSUSY Searches at CMS in the Fully Hadronic Channel
SUSY Searches at CMS in the Fully Hadronic Channel Project B2 - Supersymmetry at the Large Hadron Collider Christian Autermann, Sergei Bobrovskyi, Ulla Gebbert, Kolja Kaschube, Friederike Nowak, Benedikt
More informationThe Compact Muon Solenoid Experiment. Conference Report. Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland
Available on CMS information server CMS CR -2013/016 The Compact Muon Solenoid Experiment Conference Report Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland 18 January 2013 (v2, 21 January 2013)
More informationNon-Standard Higgs Decays
Non-Standard Higgs Decays David Kaplan Johns Hopkins University in collaboration with M McEvoy, K Rehermann, and M Schwartz Standard Higgs Decays Standard Higgs Decays 1 _ bb 140 GeV WW BR for SM Higgs
More informationCollider Physics Analysis Procedures
Collider Physics Analysis Procedures Alex Tapper Slides available at: http://www.hep.ph.ic.ac.uk/~tapper/lecture.html Aim Overview of analysis techniques at CMS Contrast with Tevatron (see DØ lecture)
More informationPhysics at the Tevatron. Lecture IV
Physics at the Tevatron Lecture IV Beate Heinemann University of California, Berkeley Lawrence Berkeley National Laboratory CERN, Academic Training Lectures, November 2007 1 Outline Lecture I: The Tevatron,
More informationSearches for electroweak production of supersymmetric gauginos and sleptons with the ATLAS detector
Searches for electroweak production of supersymmetric gauginos and sleptons with the ATLAS detector Christopher Bock on behalf of the ATLAS Collaboration SUSY5 - August 7, 5 Introduction Outline Introduction
More informationElectroweak Measurements at LHCb!
Electroweak Measurements at LHCb! Simone Bifani University of Birmingham (UK) on behalf of the LHCb collaboration LHCb workshop on quantum interference effects, QCD measurements and generator tuning CERN,
More informationStandard Model physics with taus in ATLAS
Standard Model physics with taus in ATLAS IFJ PAN, Cracow, Poland Why we are interested in taus? Tau leptons play an important role in the physics program of the ATLAS experiment as they are tools in many
More informationSupersymmetry at the LHC: Searches, Discovery Windows, and Expected Signatures
Supersymmetry at the LHC: Searches, Discovery Windows, and Expected Signatures Darin Acosta representing ATLAS & Outline Introduction to SUSY, LHC, and the Detectors Non-Higgs sparticle searches: Trigger
More informationWhat the LHC Will Teach Us About Low Energy Supersymmetry
What the LHC Will Teach Us About Low Energy Supersymmetry Darin Acosta representing ATLAS & Outline Introduction to SUSY, LHC, and the Detectors Trigger strategies at start-up Inclusive squark/gluino searches
More informationPoS(CHARGED2008)005. Charged Higgs Searches with D0. Phillip Gutierrez. University of Oklahoma
University of Oklahoma E-mail: pgutierrez@ou.edu DØ has performed a number of searches for the charged Higgs boson in the mass range 8 to 3 GeV. For masses less than the top-quark mass two methods have
More informationHiggs search in WW * and ZZ *
Higgs search in WW * and ZZ * Emanuele Di Marco on behalf of CMS collaboration La Sapienza Università di Roma & INFN Roma1 July, 29 2011 1 Higgs production at LHC gluon fusion (gg H) gg H is the dominant
More informationRare and Exotic Decays of Higgs boson
Rare and Exotic Decays of Higgs boson Kajari Mazumdar Tata Institute of Fundamental Research Mumbai Plan of talk Status of measurements for standard model Higgs boson Example of a rare decay Search for
More informationATLAS-CONF October 15, 2010
ATLAS-CONF-2010-096 October 15, 2010 Data-driven background estimation for the H τ + τ τ h search at 7 TeV with the ATLAS detector Ian Howley 7 December 2010 1 Motivation One of the primary LHC physics
More informationEvidence for Higgs Boson Decays to a Pair of τ-leptons
Evidence for Higgs Boson Decays to a Pair of τ-leptons ET miss = 119 GeV μ (pt=6 GeV) τhad (pt=96 GeV) mττ =19 GeV Nils Ruthmann mjj =65 GeV Nils Ruthmann (Universität Freiburg) On Behalf of the ATLAS
More informationDiscovery potential for SUGRA/SUSY at CMS
Discovery potential for SUGRA/SUSY at CMS Stefano Villa, Université de Lausanne, April 14, 2003 (Based on talk given at SUGRA20, Boston, March 17-21, 2003) Many thanks to: Massimiliano Chiorboli, Filip
More informationJet reconstruction in LHCb searching for Higgs-like particles
Jet reconstruction in LHCb searching for Higgs-like particles Alessandro Camboni (on behalf of LHCb Collaboration) DISCRETE'08 Valencia Dec 12th, 2008 Motivation Jet reconstruction is important for searches
More informationFirst V+jets results with CMS. Vitaliano Ciulli (Univ. & INFN Firenze) V+jets workshop, 8-10 Sep 2010, Durham
First V+jets results with CMS Vitaliano Ciulli (Univ. & INFN Firenze) V+jets workshop, 8- Sep 20, Durham Outline Jet and missing energy reconstruction W and Z selections and cross-section measurement First
More informationPhysics at Tevatron. Koji Sato KEK Theory Meeting 2005 Particle Physics Phenomenology March 3, Contents
Physics at Tevatron Contents Koji Sato KEK Theory Meeting 5 Particle Physics Phenomenology March 3, 5 mass measurement Top physics cross section Top mass measurement SM Higgs search Tevatron Run II Started
More informationHighlights of top quark measurements in hadronic final states at ATLAS
Highlights of top quark measurements in hadronic final states at ATLAS Serena Palazzo 1,2,, on behalf of the ATLAS Collaboration 1 Università della Calabria 2 INFN Cosenza Abstract. Measurements of inclusive
More informationBoosted Top Resonance Searches at CMS
Boosted Top Resonance Searches at CMS Justin Pilot, UC Davis on behalf of the CMS Collaboration Northwest Terascale Workshop, Using Jet Substructure University of Oregon 5 April 013 Introduction Many new
More informationW and Z boson production in p p collisions from Run II of the Tevatron Collider
W and Z boson production in p p collisions from Run II of the Tevatron Collider P. Petroff To cite this version: P. Petroff. W and Z boson production in p p collisions from Run II of the Tevatron Collider.
More informationFirst physics with the ATLAS and CMS experiments. Niels van Eldik on behalf of the ATLAS and CMS collaborations
First physics with the ATLAS and CMS experiments Niels van Eldik on behalf of the ATLAS and CMS collaborations Content Status of the LHC and the ATLAS and CMS experiments Event production rates First physics
More informationSearches for SUSY in events with di-leptons at CMS
Searches for SUSY in events with di-leptons at CMS SUSY 22, Beijing Daniel Sprenger. Physikalisches Institut B RWH Aachen University 7.8.22 SUSY Searches in Di-lepton Events at CMS Why di-leptonic final
More informationSearches for New Physics with Tau Leptons at the ATLAS Detector. Katharine Leney University of the Witwatersrand
Searches for New Physics with Tau Leptons at the ATLAS Detector Katharine Leney University of the Witwatersrand Overview Introduction: ATLAS and the LHC The Standard Model and beyond Tau leptons ATLAS
More informationSearch for a heavy scalar boson decaying into a pair of Z bosons in the 2l2ν final state in CMS
Search for a heavy scalar boson decaying into a pair of Z bosons in the 2l2ν final state in CMS Li Yuan Beihang University CLHCP 2016 December 18, 2016 1 Outline Introduction Overview Analysis Strategy
More informationStudy of supersymmetric tau final states with Atlas at LHC: discovery prospects and endpoint determination
Study of supersymmetric tau final states with Atlas at LHC: discovery prospects and endpoint determination University of Bonn Outlook: supersymmetry: overview and signal LHC and ATLAS invariant mass distribution
More informationRecent Results on New Phenomena and Higgs Searches at DZERO
Recent Results on New Phenomena and Higgs Searches at DZERO Neeti Parashar Louisiana Tech University Ruston, Louisiana U.S.A. 1 Outline Motivation for DØ Run II Detector at Fermilab The Fermilab Tevatron
More informationResults on Tau Physics from BaBar
Results on Tau Physics from BaBar Eric Torrence University of Oregon Search for Lepton Flavor Violation Study of τ 3h 2h + ν τ (5 prong) Tau Lifetime The BaBar Experiment Integrated Luminosity (fb -1 )
More informationZ boson studies at the ATLAS experiment at CERN. Giacomo Artoni Ph.D Thesis Project June 6, 2011
Z boson studies at the ATLAS experiment at CERN Giacomo Artoni Ph.D Thesis Project June 6, 2011 Outline Introduction to the LHC and ATLAS ((Very) Brief) Z boson history Measurement of σ Backgrounds Acceptances
More informationSearch for physics beyond the Standard Model at LEP 2
Search for physics beyond the Standard Model at LEP 2 Theodora D. Papadopoulou NTU Athens DESY Seminar 28/10/03 1 Outline Introduction about LEP Alternatives to the Higgs mechanism Technicolor Contact
More information7. Data and Monte Carlo Samples
7. and Monte Carlo Samples he data sample for the analyses presented in this document was collected between April 00 and August 007 with the DØ detector. he first part of this chapter gives an overview
More informationSearch for SUSY at CMS in lepton or photon final states. PANIC 2011 K. Theofilatos (on behalf of CMS)
Search for SUSY at CMS in lepton or photon final states CMS in one slide Optimal design for reconstructing leptons & photons Compact & precisely aligned detector with B=3.8 T Calorimeters operating inside
More informationHeavy MSSM Higgses at the LHC
Heavy MSSM Higgses at the LHC P.Vanlaer, IIHE Brussels (CMS), for the Atlas and CMS collaborations SUSY02, Hamburg, June 17-23, 2002 Outline LHC, Atlas and CMS A,H H + Conclusions SUSY02, Hamburg, June
More informationUpgrade of ATLAS and CMS for High Luminosity LHC: Detector performance and Physics potential
IL NUOVO CIMENTO 4 C (27) 8 DOI.393/ncc/i27-78-7 Colloquia: IFAE 26 Upgrade of ATLAS and CMS for High Luminosity LHC: Detector performance and Physics potential M. Testa LNF-INFN - Frascati (RM), Italy
More informationRecent Results from CDF. Gabriele Compostella (INFN and University of Padova) on behalf of the CDF Collaboration
Recent Results from CDF Gabriele Compostella (INFN and University of Padova) on behalf of the CDF Collaboration XCVI Congresso Nazionale della Società Italiana di Fisica - Bologna, 20-24 Settembre, 2010
More informationHighlights of Higgs Physics at LEP
hep-ph/43 February 4 Highlights of Higgs Physics at André Sopczak Lancaster University arxiv:hep-ph/43 v Feb 4 Abstract Final results from the combined data of the four experiments AH,, L3 and OPAL on
More informationOverview of the Higgs boson property studies at the LHC
Overview of the Higgs boson property studies at the LHC Giada Mancini, a, Roberto Covarelli b a LNF-INFN and University of Roma Tor Vergata, b INFN and University of Torino E-mail: giada.mancini@lnf.infn.it,
More informationInclusive. W & Z measurements in CMS. Georgios Daskalakis. on behalf of CMS Collaboration. .C.S.R. Demokritos
Inclusive W & Z measurements in CMS Georgios Daskalakis.C.S.R. Demokritos on behalf of CMS Collaboration 1 Overview LHC hopefully will be proven to be a discovery machine but before that the measurement
More informationOutline: Introduction Search for new Physics Model driven Signature based General searches. Search for new Physics at CDF
PE SU Outline: Introduction Search for new Physics Model driven Signature based General searches R Search for new Physics at CDF SUperSYmmetry Standard Model is theoretically incomplete SUSY: spin-based
More informationSLHC Physics Impact Albert De Roeck/CERN
SLHC Physics Impact Albert De Roeck/CERN XXXVII SLAC Summer Institute 1 Today s Lecture Contents Introduction Luminosity upgrade scenario for the LHC machine Physics with the SLHC Other possible upgrades
More informationLHC signals for SUSY discovery and measurements
06 March 2009 ATL-PHYS-SLIDE-2009-038 LHC signals for SUSY discovery and measurements Vasiliki A. Mitsou (for the ATLAS and CMS Collaborations) IFIC Valencia PROMETEO I: LHC physics and cosmology 2-6 March,
More informationSearch for top squark pair production and decay in four bodies, with two leptons in the final state, at the ATLAS Experiment with LHC Run2 data
Search for top squark pair production and decay in four bodies, with two leptons in the final state, at the ATLAS Experiment with LHC Run data Marilea Reale INFN Lecce and Università del Salento (IT) E-mail:
More informationSearch for gluino-mediated stop and sbottom pair production in events with b-jets and large missing transverse momentum
Search for gluino-mediated stop and sbottom pair production in events with b-jets and large missing transverse momentum Chiara Rizzi On behalf of the ATLAS Collaboration ALPS 2017 Obergurgl Introduction
More informationTau Reconstruction at CMS. Evan Friis
Tau Reconstruction at CMS Evan Friis Outline Taus at hadron colliders Tau ID algorithms at CMS Tau ID measurements in 2010 Z ττ standard candle SVfit: τ pair mass reconstruction MSSM H ττ Tau ID at hadron
More informationSearch for R-parity violating SUSY signatures with the ATLAS detector
Search for R-parity violating SUSY signatures with the ATLAS detector SEARCH22, Maryland Shimpei Yamamoto (Univ. of Tokyo) on behalf of the ATLAS collaboration Outline. Introduction 2. RPV-SUSY searches
More informationAnalysis of W µν+jets
Analysis of W µν+jets Introduction The detection of leptons (muons and electrons) is very important for physics at the current and higher energy regimes. The study of intermediate vector bosons decaying
More informationInclusive SUSY Searches at CMS with Emphasis on Detector Systematics
Inclusive SUSY Searches at with Emphasis on Detector Systematics R. Cavanaugh (on behalf of ) University of Florida SUSY06 Detector Background Calibrations Inclusive Search Strategies Detector Systematics
More informationSUPERSYMMETRY SEARCHES AT CDF
SUPERSYMMETRY SEARCHES AT CDF Xavier Portell Freiburg, 8 th Nov 2006 1 OUTLINE Tevatron and CDF Supersymmetry (SUSY) SUSY models phenomenology SUSY analyses at CDF: Squarks and Gluinos (Missing E T +jets)
More informationSearches for New Phenomena in Events with Multiple Leptons with the ATLAS Detector
Searches for New Phenomena in Events with Multiple Leptons with the ALAS Detector ÜLİN VAROL University of Massachusetts, Amherst On Behalf of the ALAS Collaboration OULINE Introduction Excited e/μ Search
More informationDirect Measurement of the W Total Decay Width at DØ. Outline
Direct Measurement of the W Total Decay Width at DØ Introduction Junjie Zhu University of Maryland On behalf of the DØ Collaboration Monte Carlo Simulation Event Selection Outline Determination of the
More informationSearch for Supersymmetry at CMS in all-hadronic final states
Search for Supersymmetry at CMS in all-hadronic final states The 9th Particles and Nuclei International Conference, MIT Matthias Schröder (Universität Hamburg) on behalf of the CMS Collaboration 5 July
More informationTevatron Physics Prospects. Paul Grannis, for the CDF and DØ collaborations ICFA Seminar, Oct
Tevatron Physics Prospects Paul Grannis, for the CDF and DØ collaborations ICFA Seminar, Oct. 29 2008 CDF and DØ Operations Fermilab is planning to run CDF and DØ through FY2010. The Tevatron is now delivering
More informationSearch for b Ø bz. CDF note Adam Scott, David Stuart UCSB. 1 Exotics Meeting. Blessing
Search for b Ø bz CDF note 8465 Adam Scott, David Stuart UCSB Exotics Meeting Blessing 1 Exotics Meeting Analysis in a Nutshell Looking for new particles decaying to Z+jets Select Z s in the dielectron
More informationThe HL-LHC physics program
2013/12/16 Workshop on Future High Energy Circular Collider 1 The HL-LHC physics program Takanori Kono (KEK/Ochanomizu University) for the ATLAS & CMS Collaborations Workshop on Future High Energy Circular
More informationSearch for Higgs to tt at CMS
Search for Higgs to tt at CMS Arun Nayak IRFU/SPP, CEA, Saclay 11/10/2013 Aperos du SPP 1 Why Higgs to tt? Introduction Most sensitive channel to probe lepton couplings o Important to establish SM predictions
More informationProspects for early discoveries in final states. LRSM and Leptoquarks
ν ν lq Prospects for early discoveries in final states with di-leptons, jets and no missing energy: LRSM and Leptoquarks University Of Pittsburgh On behalf of the ATLAS Collaboration The ATLAS detector
More informationElectroweak results. Luca Lista. INFN - Napoli. LHC Physics
Electroweak results Luca Lista INFN - Napoli EWK processes at LHC p p W and Z production in pp collisions proceeds mainly form the scattering of a valence quark with a sea anti-quark The involved parton
More informationVBF SM Higgs boson searches with ATLAS
VBF SM Higgs boson searches with Stefania Xella (for the collaboration) Niels Bohr Institute, Copenhagen University, Denmark E-mail: xella@nbi.dk The observation of a Standard Model Higgs boson produced
More informationDiscovery Physics at the Large Hadron Collider
+ / 2 GeV N evt 4 10 3 10 2 10 CMS 2010 Preliminary s=7 TeV -1 L dt = 35 pb R > 0.15 R > 0.20 R > 0.25 R > 0.30 R > 0.35 R > 0.40 R > 0.45 R > 0.50 10 1 100 150 200 250 300 350 400 [GeV] M R Discovery
More informationEvents with High P T Leptons and Missing P T and Anomalous Top at HERA
with High Leptons and Missing and Anomalous Top at HERA David South (DESY) On Behalf of the H Collaboration IIth International Workshop on Deep Inelastic Scattering (DIS 24) Štrbské Pleso, High Tatras,
More informationInclusive SUSY search strategies. SUSY-PAT All-hadronic SUSY search Inclusive leptonic SUSY search
1 Inclusive SUSY search strategies Early analyses (Universität Hamburg) for the SUSY group SUSY-PAT All-hadronic SUSY search Inclusive leptonic SUSY search Outline Introduction PAT Analysis Framework Trigger
More informationttbar Background Estimation in the Search for b-associated MSSM Higgs Bosons Decaying to Tau-Pairs with ATLAS DPG Bonn, T 45. Higgs
ttbar Background Estimation in the Search for b-associated MSSM Higgs Bosons Decaying to Tau-Pairs with ATLAS DPG Bonn, T 45. Higgs 17.03.2010 Jana Schaarschmidt Supervised by Michael Kobel, Wolfgang Mader
More informationSearch for Invisible Decay of Higgs boson at LHC
Search for Invisible Decay of Higgs boson at LHC Kajari Mazumdar Tata Institute of Fundamental Research Mumbai DHEP seminar, TIFR, Mumbai 22.4.2014 Plan of the talk Preliminaries Status of measurements
More informationPhysics at Hadron Colliders
Physics at Hadron Colliders Part 2 Standard Model Physics Test of Quantum Chromodynamics - Jet production - W/Z production - Production of Top quarks Precision measurements -W mass - Top-quark mass QCD
More informationProbing SUSY Contributions to Muon g-2 at LHC and ILC
Probing SUSY Contributions to Muon g-2 at LHC and ILC Motoi Endo (Tokyo) Based on papers in collaborations with ME, Hamaguchi, Iwamoto, Yoshinaga ME, Hamaguchi, Kitahara, Yoshinaga ME, Hamaguchi, Iwamoto,
More informationP. Sphicas/SSI2001. Standard Model Higgs
Standard Model Higgs SM Higgs (I) Production mechanisms & cross section Studying EWSB at the LHC 2 Decays & discovery channels Higgs couples to m f 2 SM Higgs (II) Heaviest available fermion (b quark)
More information