William Edson SUNY at Albany.  New Results for Fit:  Signal Fraction: 0.664442±0.0418289  Chi2: 29.953  Meas. Used: 31  σ : 170.884±10.7578  New.

Slides:



Advertisements
Similar presentations
William Edson SUNY at Albany Anirvan Sircar Louisiana Tech University.
Advertisements

1 Data Analysis II Beate Heinemann UC Berkeley and Lawrence Berkeley National Laboratory Hadron Collider Physics Summer School, Fermilab, August 2008.
Current limits (95% C.L.): LEP direct searches m H > GeV Global fit to precision EW data (excludes direct search results) m H < 157 GeV Latest Tevatron.
Effect of b-tagging Scale Factors on M bb invariant mass distribution Ricardo Gonçalo.
WH, H->bb MICHAEL WRIGHT, UNIVERSITY OF GLASGOW. INTRODUCTION Optimize University of Glasgow WH analysis by comparing with LMU and Wisconsin MC cut flows.
Jet Veto Scale Factor for ZZ Analysis Haijun Yang, Lailin Xu, Bing Zhou ATLAS SM ZZ  Meeting February 2, 2012.
1 Measurements at 8 TeV of TTbar events with additional particles in the final state Boris Mangano (ETH Zürich) on behalf of the CMS collaboration Boris.
The Matrix Method Data-driven method of estimating the W→lv and QCD multijet contributions to sample S’.
Top Turns Ten March 2 nd, Measurement of the Top Quark Mass The Low Bias Template Method using Lepton + jets events Kevin Black, Meenakshi Narain.
Kevin Black Meenakshi Narain Boston University
Sept 30 th 2004Iacopo Vivarelli – INFN Pisa FTK meeting Z  bb measurement in ATLAS Iacopo Vivarelli, Alberto Annovi Scuola Normale Superiore,University.
Search for B     with SemiExclusive reconstruction C.Cartaro, G. De Nardo, F. Fabozzi, L. Lista Università & INFN - Sezione di Napoli.
Update FTK Meeting 05/02/06 Erik Brubaker U of Chicago.
Jake Anderson, on behalf of CMS Fermilab Semi-leptonic VW production at CMS.
4/10/12 Contribution in ATLAS Collaboration 1 Talk “Multi-jet balance for high pT jet calibration” presented on ATLAS Hadronic Calibration Workshop 2011(SLAC.
Yu Bai (IHEP, Beijing) On behalf of the SUSY Weak Production team ACCM 23, Mar 3, 2013 Search of SUSY Weak Production with hadronic taus Search of SUSY.
Heavy charged gauge boson, W’, search at Hadron Colliders YuChul Yang (Kyungpook National University) (PPP9, NCU, Taiwan, June 04, 2011) June04, 2011,
The Physics of Generations (Update) 11-Dec-03 Don Lincoln f.
Energy Flow and Jet Calibration Mark Hodgkinson Artemis Meeting 27 September 2007 Contains work by R.Duxfield,P.Hodgson, M.Hodgkinson,D.Tovey.
William P. Edson, Teeba Rashid, Dr. Sajjad Alam 1 Dr. Dick Greenwood, Anirvan Sircar 2 Dr. Patrick Skubic, Dr. Muhammad Saleem, Dr. Brad Abbot, Dr. Phil.
A. Martyniuk a, P. Miyagawa b, M. Owen c, O. Trifis c, V. Chavda c, and U.K. Yang c a: University of Victoria b: University of Sheffield c: University.
Associated top Higgs search: with ttH (H  bb) Chris Collins-Tooth, 17 June 2008.
W+jets and Z+jets studies at CMS Christopher S. Rogan, California Institute of Technology - HCP Evian-les-Bains Analysis Strategy Analysis Overview:
1 HEP 2008, Olympia, Greece Ariadni Antonaki Dimitris Fassouliotis Christine Kourkoumelis Konstantinos Nikolopoulos University of Athens Studies for the.
August 30, 2006 CAT physics meeting Calibration of b-tagging at Tevatron 1. A Secondary Vertex Tagger 2. Primary and secondary vertex reconstruction 3.
Sensitivity Prospects for Light Charged Higgs at 7 TeV J.L. Lane, P.S. Miyagawa, U.K. Yang (Manchester) M. Klemetti, C.T. Potter (McGill) P. Mal (Arizona)
1 Hgg Cut based Analysis update Jim Branson, Chris Palmer, Marco Pieri, Matteo Sani, Sean Simon.
QCD and Top backgrounds in W+jets and Rjets Alessandro Tricoli (CERN) on behalf of W+jets and Rjets groups 3 rd May 2013 W+jets and Rjets EB Meeting.
Timescale The nominal dates for SM approvals for EPS are June 30 and July 7 for the Plenary meetings, with availability of a draft supporting note to the.
William Edson SUNY at Albany.  New Results for Fit:  Signal Fraction: ±  Chi2:  Meas. Used: 31  σ : ±  New.
Slides for EB3. Left Problems from EB2 1. Why muon triggers are not used in e  channel? 2. Add backgrounds estimation for signal search region 3. Add.
W/Z+Jets production studies in ATLAS
Measurement on the mass difference between top and anti-top quarks Vikash Chavda 1, Un-Ki Yang 1, Jahred Adelman 2 University of Manchester 1, Yale University.
QCD Background Estimation From Data Rob Duxfield, Dan Tovey University of Sheffield.
Jet + Isolated Photon Triple Differential Cross Section Nikolay Skachkov: “Photon2007”, Paris, 9-13 July 2007 DO Measurement of Triple Differential Photon.
Tomas Hreus, Pascal Vanlaer Overview: K0s correction stability tests Jet-pt correction closure test Study of Strangeness Production in Underlying Event.
Tomas Hreus, Pascal Vanlaer Study of Strangeness Production in Underlying Event at 7 TeV 1QCD low pT meeting, 18/03/2011.
Jet + Isolated Photon Triple Differential Cross Section Nikolay Skachkov: “Photon2007”, Paris, 9-13 July 2007 DO Measurement of Triple Differential Photon.
Stano Tokar, slide 1 Top into Dileptons Stano Tokar Comenius University, Bratislava With a kind permissison of the CDF top group Dec 2004 RTN Workshop.
Z  BF using  hadronic events Silke Duensing Aug 8th, 2003.
EPS Manchester Daniela Bortoletto Associated Production for the Standard Model Higgs at CDF D. Bortoletto Purdue University Outline: Higgs at the.
Bc → J/   Lifetime measurement Use 6.7 fb -1 and try two independent approaches Selection 1: no dependence of selection on decay time Fit fixes bkgd.
The Univ. of Tokyo Dept. of Physics 1 New MT method to remove SUSY contaminations CSC Note 1&2 : 27 Aug 2007 Ginga Akimoto, Y. Kataoka, S. Asai The University.
Wuppertal ttbar strategy meeting 16 August 2012, T. Cornelissen 1 Sebastian, Thijs Status of JetElectron QCD fit in resonance analysis.
1 UCSD Meeting Calibration of High Pt Hadronic W Haifeng Pi 10/16/2007 Outline Introduction High Pt Hadronic W in TTbar and Higgs events Reconstruction.
I'm concerned that the OS requirement for the signal is inefficient as the charge of the TeV scale leptons can be easily mis-assigned. As a result we do.
Viktor Veszpremi Purdue University, CDF Collaboration Tev4LHC Workshop, Oct , Fermilab ZH->vvbb results from CDF.
1 RA1 Analysis Exclusive n-jet + MET search Overview and Status Report Tanja Rommerskirchen on behalf of the RA1 group Universitaet Zuerich SUSY Workshop;
Search for Standard Model Higgs in ZH  l + l  bb channel at DØ Shaohua Fu Fermilab For the DØ Collaboration DPF 2006, Oct. 29 – Nov. 3 Honolulu, Hawaii.
H->WW->lνlν Analysis - Improvements and results - - Data and MC - Higgs Working group meeting, 6 January 2011 Magda Chełstowska & Rosemarie Aben.
Upsilon production and μ-tagged jets in DØ Horst D. Wahl Florida State University (DØ collaboration) 29 April 2005 DIS April to 1 May 2005 Madison.
Investigation on CDF Top Physics Group Ye Li Graduate Student UW - Madison.
QCD estimate with the matrix method Alexander D. with the help of many…
Status of the Higgs to tau tau analysis Carlos Solans Cristobal Cuenca.
Andy Haas D0 Columbia Meeting Slide 1 Top mass, ME, lepton+jets, p17 ● e/mu pt>20, met>20, 4 jets pt>20 ● triangle cuts to remove QCD ● >=1 NN b-tagged.
1 QCD fits via TFractionFitter ● I took another look at the QCD fit problem: ● A fraction of the fits hangs in an infinite loop ● A (smaller) fraction.
2nd lepton veto, in the one-lepton SUSY analysis
CMSSW_3_1_1 preproduction samples
Report from SUSY working group
Missing ET with the First Data: Wl (l=e,)
ttbar τ + jets: Update on QCD Estimation
CDS comments on supporting note
Stop->4 bodies signal samples with 2 leptons in final state
Uncertainties on top quark mass due to modeling
2vtx tagged dijets mass resolution study
Observation and measurement of HW+W-
Measurement of
Dilepton Mass. Progress report.
Higgs  update Catalin and Tony May 22, 2007
Northern Illinois University / NICADD
Presentation transcript:

William Edson SUNY at Albany

 New Results for Fit:  Signal Fraction: ±  Chi2:  Meas. Used: 31  σ : ±  New Corrected Results:  Signal Fraction: ±  σ : ±  Correction Systematic: ±

SampleFractionCor. Fraction σ Unc (absolute)Unc (%) Nominal JER JRE JES up JES down JVF up JVF down BSF up BSF down MET up MET down Tau trig up Tau trig down TES up TES down Tau Eveto SF up Tau Eveto SF down

Nominaltes_uptes_down No cut GRL Trigger ntrack > Electron/muon overlap Event cleaning Lepton veto ntaus > njets ≥ MET > 60 GeV MT < 80 GeV nbjets > Trigger match Truth match Cutflows

SampleFractionCor. Fraction σ Unc (absolute)Unc (%) Nominal Wnorm Up Wnorm Down QCD Bin/Range HiISR LowISR

SampleFractionCor. Fraction σ Unc (absolute)Unc (%) Nominal Original kfac/ σ (FE) from TopMC11 twiki Correction using Ref σ ’s Using kfac/ σ (FE) from

SampleFractionCor. Fraction σ Unc (absolute)Unc (%) Nominal AlpHerwig (baseline) (105200) SYST_AtF_ SYST_AtF_ SYST_Full_ ) fullsim mc11c POWHEG+fPythia sample (SYST_Full_117050) and sample ) fullsim mc11c POWHEG+fPythia sample (SYST_Full_117050) and the fullsim mc11c ALPGEN+HERWIG samples (AlpHerwig(baseline)) 1.3) AtlFast2 mc11b POWHEG+fPythia sample (SYST_AtF_117050) POWHEG+fHerwig sample (SYST_AtF_105860)

SampleFractionCor. Fraction σ Unc (absolute)Unc (%) Nominal > <

MET Dijet Mass

MET Dijet Mass

for (unsigned int tfj = (tau_matched.size() - 1); tfj > 0; tfj--) { try { int REFN1 = tau_matched.at(tfj).entry(); int REFN2 = tau_matched.at(tfj-1).entry(); if( (physics->tau_BDTJetScore->at(REFN1)) > (physics- >tau_BDTJetScore->at(REFN2))) { save = tau_matched.at(tfj); tau_matched.at(tfj) = tau_matched.at(tfj-1); tau_matched.at(tfj-1) = save; } catch (const std::out_of_range& C12_2){ std::cerr << endl << "C12.2: OUT OF RANGE ERROR: " << C12_2.what() << endl; EMERXIT = 12; continue; }

SampleFractionCor. Fraction σ Unc (absolute) Unc (%) Nominal Range Range Range Range Range Range Bins Bins Bins Bins Range increases/decreases in steps of 20GeV Bin amount increases/decreases in steps of 5

 Y(0): ±  Slope: ±  Chi2: NDF: 8998

Slope: ± y-intercept: ± Chi2: NDF: 7

Input Fraction Previous Gaussian Mean Output Fraction Unc.Gaussian Mean Output Fraction Unc

RangeFit to MeansFit to All ValuesCorrected σ Y(0)SlopeY(0)Slope 0.1 – – – –

MC Tau Count MC Tau Children pdgIDMC Tau Children Count Leptonic pdgID values: e → 11, μ → 13, τ → 15

Samples Normalized to Own Integrals Samples Normalized to Sum of Integrals

 C0: GRL  C1: Trigger  C2: Primary vertex with ntracks > 4  C3: Electron/muon overlap  C4: Jet cleaning  C5: Lepton Veto  C6: tau n ≥ 1  C7: n jets >= 4 with eta 0.75  C8: MET > 60GeV  C9: M T < 80GeV  C10: >= 1 b jet  C11: Trigger matched tau n ≥ 1 and p T >= 40GeV  C12: MC tau object match

 Equation:  N(x): total number of events of type x for distribution  n(x) i : number of events in bin of type x  frac(Sig): fraction of N(Remain) expected to be Signal  binfrac(x) i : fraction of events in bin of type x expected from MC or template  σ i : uncertainty in bin i

 σ i determined using factors for:  bin error:  data  signal, MC  QCD template  other backgrounds, MC  statistical error:  data: signal region  other backgrounds, MC  signal, MC  QCD template (uncertainty of background region data and all MC background region carried through via default SumW2

 Results for plot:  chi-square:  p-value:  ndf: 14  chi/ndf:

 Results for plot:  chi-square:  p-value:  ndf: 15  chi/ndf:

 Results for plot:  chi-square:  p-value:  ndf: 18  chi/ndf:

 Results for plot:  chi-square:  p-value:  ndf: 12  chi/ndf: 1.323

 Results for plot:  chi-square:  p-value:  ndf: 11  chi/ndf: 1.308

CutSig EvtsFakesSig Eff.Fake Ratio Rej Fact. Sig/ sqrt(Bkgd) Sig/ Sqrt(Sig+ Bkgd) C5 Lep Veto C6 ntaus > C7 njets C8 MET C9 MT C10 bjet C12 Trig match