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WWZRun3
(18 Jan 2024,
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WWZ Run 3 Analysis %TOC% ---++ Meetings (weekly) *Thursday, 7:00 am (CA) / 10:00 am (FL) / 4:00 pm (CERN) %BR% Meetings are held in [[https://ufl.zoom.us/my/p.chang][Philip's Zoom room]] Indico [[https://indico.cern.ch/event/1312765/][agenda]] --- ---++ Presentations <br />%EDITTABLE{}% | *Date* | *Keyword* | *Meeting* | *Who* | *Title* | *Summary* | *Link* | *Comments* | | 5/22/23 | Tau ID vs Jets (follow up) | Weekly Meeting | Keegan | Tau ID vs jets (follow up) | Gen-matching study to estimate fake contribution in tau SRs | [[https://docs.google.com/presentation/d/1S6nvAvmY6Ukhoz2TH_DQtxA5X8JlD32yiAjN7PrEIGg/edit?usp=sharing][slides]] | ... | | 5/16/23 | Tau ID vs Jets | None | Keegan | Tau ID vs jets | Yields comparison for DeepTau ID WPs vs jets | [[https://docs.google.com/presentation/d/1S6nvAvmY6Ukhoz2TH_DQtxA5X8JlD32yiAjN7PrEIGg/edit#slide=id.p][slides]] | ... | | 5/15/23 | Tau ID vs Leps | Weekly Meeting | Keegan | Tau ID vs e/mu | Yields comparison for different DeepTau IDs vs light leptons | [[https://docs.google.com/presentation/d/10guWhn1UlVlRsqS-sMKv7w6r4G5ynJzNE0LDOznt5VM/edit#slide=id.p][slides]] | ... | | 5/15/23 | Run3 DiMuon Analysis | Weekly Meeting | Matthew | Run3 DiMuon | MC and Data Comparison for DiMuon Triggered Events in Run3 era G | [[https://drive.google.com/file/d/16zt3SpKR7MtwEZ_qVGfqnsXSzoah_s4q/view?usp=share_link][slides]] | ... | | 5/09/23 | Keegan's ATC Talk | None | Keegan | WWZTo4L Advancement Talk | Summary of the status of the WWZ->4L analysis | [[https://docs.google.com/presentation/d/17WQvBXTdEfVgWyTSTV9wn91aeym-aTsIKCl4CTiBia4/edit#slide=id.p][slides]] | ... | | 5/3/23 | Tau Channels | None | Keegan | Tau Final States | Preliminary yields for tau final states and comparison with light lepton final states | [[https://docs.google.com/presentation/d/1Pe500kIsp57KEBHoQ7L9N0GsDxfGvGucD61XISJ3U2c/edit#slide=id.p][slides]] | ... | | 3/13/23 | Lepton pT | Weekly Meeting | Keegan | Lepton pT optimization | Comparison of yields in SR for different lepton pT thresholds | [[http://cern.ch/go/6CZp][slides]] | ... | | 3/6/23 | Signal xsec | Weekly Meeting | Keegan | Signal xsec | Comparison of cross sections for inclusive vs 4l sample | [[http://cern.ch/go/rcH6][slides]] | ... | | 2/13/22 | Lepton ID Study | Weekly Meeting | Keegan | Lepton ID Study | Comparison of yields for new vs old lepton IDs | [[http://cern.ch/go/8QmM][slides]] | ... | | 12/15/22 | pfMET vs PuppiMET | None | Keegan | Signal Efficiency for pfMET and PuppiMET | Determined cut on PuppiMET for optimal signal efficiency | [[http://cern.ch/go/9pLN][slides]] | ... | | 12/08/22 | pfMET vs PuppiMET (cont.) | Weekly Meeting | Keegan | Background MET distribution | Compared data/background yields for pfMET vs PuppiMET | [[http://cern.ch/go/f66z][slides]] | ... | | 12/1/2022 | Lepton ID | Weekly Meeting | Matthew | Lepton ID Study | made Loose/Z/W Candidate Efficiency plots for e/µ in pt v. eta | [[http://cern.ch/go/b6Rq][slides]] | ... | | 12/1/2022 | pfMET vs PuppiMET | Weekly Meeting | Keegan | MET in ZZ CR | Compared data/ZZ background for PuppiMET vs pfMET in ZZ control region | [[http://cern.ch/go/FCX6][slides]] | ... | | 11/17/2022 | ZZ Background | Weekly Meeting | Keegan | ZZ Background Yields | Compared ZZ background yields in ZZ CR between NanoAOD and MiniAOD | [[http://cern.ch/go/Lhf8][slides]] | ... | | 11/10/22 | Signal Yields | Weekly Meeting | Keegan | Signal Yields | Comparison of signal yield between NanoAOD and MiniAOD | [[http://cern.ch/go/PB6F][slides]] | ... | ---++ People Claudio Campagnari (UCSB)%BR% Philip Chang (UF)%BR% Keegan Downham (UCSB)%BR% Matthew Dittrich (UF)%BR% --- ---++ Data and MC Samples A google spreadsheet containing the list of short names for all samples used in the analysis can be found [[https://docs.google.com/spreadsheets/d/1fTy4CwRkBf9XlJiudEtcUwJPKTbZuhKpFLmQjbb7TnE/edit#gid=0][here]] The full list of samples (will full sample names) can be found [[https://github.com/cmstas/VVVNanoLooper/blob/698c634d97ae7aaf4febb6ce37291b2a74e2230d/analysis/run_analyzer.py][here]]. --- ---++ Skimming There will be 2 sets of skims for 2016-2018 data/MC: an inclusive 4-lepton skim and a 3-lepton skim. For a first skim, the selected leptons will satisfy the following criteria * *Muons* * looseId = 1 * |η| < 2.4 * p<sub>T</sub> > 10 GeV * pfIsoId >= 1 * *Electrons* * mvaFall17V2noIso_WPL = 1 * |η| < 2.5 * p<sub>T</sub> > 10 GeV * pfRelIso03_all < 0.4 Skims for signal and background MC can be found in Keegan's ceph area on UAF: */ceph/cms/store/user/kdownham/skimOutput/WWZ_4L/* A new set of skims, made for the purposes of testing the new lepton ID (see pre-selection for details), has been made. This is an inclusive 4-lepton selection that requires * *Muons* * miniPFRelIso_all < 0.4 * mediumId = true * |η| < 2.4 * p<sub>T</sub> > 10 GeV * *Electrons* * miniPFRelIso_all < 0.4 * |η| < 2.5 * p<sub>T</sub> > 10 GeV Skims for testing the new lepton ID can be found in Keegan's ceph area on UAF: */ceph/cms/store/user/kdownham/skimOutput/WWZ_newLepID/* ---++++ Most recent version The most up-to-date version of the skims is an inclusive 3-lepton skim that is used for both the 3-lepton+tau and 4-lepton analyses. It can be found in Keegan's storage area on ceph in the following directory: */ceph/cms/store/user/kdownham/skimOutput/3LepTau_4Lep/* This set of skims is compatible with the new lepton ID (TOP-UL MVA ID) and utilizes the following selection criteria for leptons: * 3 or more leptons (electrons or muons) satisfying --- ---++ Pre-Selection (Old Lepton ID) This analysis targets the 4-lepton final state. The pre-selection criteria is as follows: * *Preselection*: exactly 4 leptons satisfying the Common veto ID (see section "Skimming" for the definition) * *Lepton IDs*: Leptons are categorized as a Z-candidate or a W-candidate. The criteria for electron and muon IDs for W and Z candidates are * *Electrons* * *Z candidate (ZID)* * ID: MVA POG Loose NoIso * |IP<sub>3D</sub>/σ<sub>IP<sub>3D</sub></sub>| < 4 * I<sub>rel,R=0.3,EA,Lep</sub> < 0.2 (Not used) * *W candidate (WID)* * ID: MVA 90% Iso * |IP<sub>3D</sub>/σ<sub>IP<sub>3D</sub></sub>| < 4 * I<sub>rel,R=0.3,EA,Lep</sub> < 0.2 (Not used) * *Muons* * *Z candidate (ZID)* * ID: Medium * |IP<sub>3D</sub>/σ<sub>IP<sub>3D</sub></sub>| < 4 * I<sub>rel,R=0.4,Δβ</sub> < 0.25 * *W candidate (WID)* * ID: Medium * |IP<sub>3D</sub>/σ<sub>IP<sub>3D</sub></sub>| < 4 * I<sub>rel,R=0.4,Δβ</sub> < 0.15 * *Z Candidate Selection*: The pair of leptons passing the ZID requirement with same flavor, opposite charge, that have an invariant mass closest to the Z boson mass. Both leptons are also subject to the following p<sub>T</sub> and m<sub>ll</sub> requirements: * leading Z candidate lepton: p<sub>T</sub> > 25 GeV * subleading Z candidate lepton: p<sub>T</sub> > 15 GeV * |m<sub>ll</sub> - m<sub>Z</sub>| < 10 GeV * *W Candidate Selection*: The remaining two leptons (the non-Z candidates) passing the WID requirements are then chosen as the W lepton candidates. We require the W lepton candidates to have opposite charge. Both leptons are subject to the following p<sub>T</sub> requirements: * leading W candidate lepton: p<sub>T</sub> > 25 GeV * subleading W candidate lepton: p<sub>T</sub> > 15 GeV * *QCD low mass resonance veto*: Any opposite charge pair of leptons must have an invariant mass > 12 GeV * *b-tagged jet veto*: selected events must have no b-tagged jets --- ---++ Pre-Selection (New Lepton ID) This analysis targets the 4-lepton final state. The selection for leptons is as follows: * *Preselection*: exactly 4 leptons satisfying the following criteria * *Muons*: * p<sub>T </sub> > 10 GeV * |η| < 2.4 * |d<sub>xy</sub>| < 0.05 cm * |d<sub>z</sub>| < 0.1 cm * |IP<sub>3D</sub>/σ<sub>IP<sub>3D</sub></sub>| < = 8 * miniPFRelIso_all < 0.4 * mediumId = true * MVA score > 0.64 * *Electrons*: * p<sub>T</sub> > 10 GeV * |η| < 2.5 * |d<sub>xy</sub>| < 0.05 cm * |d<sub>z</sub>| < 0.1 cm * |IP<sub>3D</sub>/σ<sub>IP<sub>3D</sub></sub>| < = 8 * miniPFRelIso_all < 0.4 * lostHits < = 1 * convVeto = true * tightCharge = 2 * MVA score > 0.81 * <strong>Lepton p<sub>T </sub>: </strong>We require the leading (subleading) lepton in the event to have p<sub>T</sub> > 25 (15) GeV. The third and fourth leptons in the event are both required to have p<sub>T</sub> > 10 GeV.<sub style="font-weight: bold;"> </sub> * *Z Candidate Selection*: The pair of leptons passing the above Preselection requirement with same flavor, opposite charge, that have an invariant mass closest to the Z boson mass. Both leptons are also subject to the following requirements: * |m<sub>ll</sub> - m<sub>Z</sub>| < 10 GeV * both leptons: |IP<sub>3D</sub>/σ<sub>IP<sub>3D</sub></sub>| < 4 * for electrons: relIso03_all < 0.2 * *W Candidate Selection*: The remaining two leptons (the non-Z candidates) passing the above Preselection requirements are then chosen as the W lepton candidates. We require the W lepton candidates to have opposite charge. Both leptons are subject to the following additional requirements: * both leptons: |IP<sub>3D</sub>/σ<sub>IP<sub>3D</sub></sub>| < 4 * for electrons: relIso03_all < 0.2 * *QCD low mass resonance veto*: Any opposite charge pair of leptons must have an invariant mass > 12 GeV * *b-tagged jet veto*: selected events must have no b-tagged jets * b-tagged jets: jets passing loose WP of btagDeepB algorithm ---++ Event Categorization Events passing the pre-selection are categorized according to the flavors of the W candidate leptons. Two categories are defined: the opposite flavor category (eμ) and the same flavor category (ee/μμ). Below is a brief description of the dominant backgrounds in each category and the selections made to address said backgrounds: * *eμ:* The main backgrounds in this category are ZZ--> ττ --> eμ (for m<sub>ll,Wcands</sub> < 100 GeV) and ttZ (for m<sub>ll,Wcands</sub> > 100 GeV). The ZZ background is reduced heavily by cutting on the m<sub>T2</sub> variable, while the ttZ background is largely unaffected by cutting on m<sub>T2</sub> due to the similar kinematics as the signal. Because of this, events with m<sub>ll,Wcands</sub> < 100 GeV are required to have m<sub>T2</sub> > 25 GeV, while events with m<sub>ll,Wcands</sub> > 100 GeV are not subject to any cut on m<sub>T2</sub>. * *ee/μμ:* The main background in this category is ZZ--> 4l. No additional selection is applied to this category prior to binning (see sec. "Binning"). --- ---++ Signal Regions Events in the eμ (ee/μμ) category are further separated into four (three) signal regions (SRs) based on m<sub>ll,Wcands</sub> (p<sub>T,miss</sub>, p<sub>T,4l</sub>). The signal regions for both categories are given below: * *ee/μμ:* * Bin A: p<sub>T,miss</sub> > 120 GeV * Bin B: 70 GeV < p<sub>T,miss</sub> < 120 GeV, 40 GeV < p<sub>T,4l</sub> < 70 GeV * Bin C: 70 GeV < p<sub>T,miss</sub> < 120 GeV, 70 GeV < p<sub>T,4l</sub> * *eμ:* * Bin 1: 0 GeV < m<sub>ll,Wcands</sub> < 40 GeV * Bin 2: 40 GeV < m<sub>ll,Wcands</sub> < 60 GeV * Bin 3: 60 GeV < m<sub>ll,Wcands</sub> < 100 GeV * Bin 4: 100 GeV < m<sub>ll,Wcands</sub> --- ---++ Preliminary (Baseline) Results ---++++ Cut Based Analysis (4-lepton channel) All plots for the baseline selection are stored [[http://uaf-10.t2.ucsd.edu/~kdownham/WWZ/070623_masterSync/Run2/][here]] on Keegan's public UAF area The vvvtrees used to get these numbers are in the following area of Keegan's UAF directory: */ceph/cms/store/user/kdownham/VVVAnalysis/070623_masterSync/* The baseline yields in the 4-lepton signal regions are as follows: | SR Bins | NonResonant WWZ (signal) | ZH (signal) | ∑bkgds | ZZ | ttZ | Higgs | WZ | Other | | 1 | 0.694 ± 0.005 | 3.234 ± 0.012 | 1.528 ± 0.188 | 0.894 ± 0.023 | 0.339 ± 0.031 | 0.181 ± 0.168 | 0.107 ± 0.076 | 0.007 ± 0.007 | | 2 | 0.796 ± 0.005 | 1.437 ± 0.008 | 1.787 ± 0.198 | 1.083 ± 0.026 | 0.442 ± 0.034 | 0.237 ± 0.193 | 0 ± 0 | 0.024 ± 0.009 | | 3 | 1.574 ± 0.007 | 0.379 ± 0.004 | 1.753 ± 0.224 | 0.668 ± 0.020 | 0.864 ± 0.051 | -0.059 ± 0.164 | 0.176 ± 0.133 | 0.103 ± 0.052 | | 4 | 5.310 ± 0.013 | 0.159 ± 0.004 | 3.949 ± 0.261 | 0.550 ± 0.018 | 2.586 ± 0.090 | 0.475 ± 0.167 | 0.240 ± 0.170 | 0.100 ± 0.052 | | 5 | 2.513 ± 0.009 | 1.078 ± 0.009 | 3.833 ± 0.244 | 1.595 ± 0.031 | 1.486 ± 0.066 | 0.701 ± 0.230 | 0 ± 0 | 0.052 ± 0.038 | | 6 | 1.836 ± 0.008 | 1.417 ± 0.010 | 6.386 ± 0.277 | 5.050 ± 0.054 | 1.032 ± 0.057 | 0.294 ± 0.265 | 0 ± 0 | 0.011 ± 0.009 | | 7 | 0.560 ± 0.004 | 0.690 ± 0.005 | 3.992 ± 0.150 | 3.716 ± 0.046 | 0.242 ± 0.029 | 0.024 ± 0.139 | 0 ± 0 | 0.009 ± 0.007 | <strong>Combined Significance: </strong>using signal+background MC in the 4-lepton SRs, we obtain a combined significance of <strong>4.46σ </strong>(via Higgs Combine Tool) --- ---++ BDT Analysis ---+++ BDT Training Information: To provide better rejection against the major backgrounds (ZZ and ttZ), a total of 4 different BDTs are trained (2 per signal process, and 2 per channel). Enumerating this, we have: * WWZ vs Backgrounds (ZZ,ttZ) in the opposite-flavor channel * ZH vs Backgrounds (ZZ,ttZ) in the opposite-flavor channel * WWZ vs Backgrounds (ZZ,ttZ) in the same-flavor channel * ZH vs Backgrounds (ZZ,ttZ) in the same-flavor channel For the first version of the BDT (v1), the important information is listed below: * List of input variables that were trained on is [[http://uaf-10.t2.ucsd.edu/~kdownham/WWZ/BDT_Information/v1/inputs/Input_Vars_List_v1.pdf][here]] * xml files containing the weights for the [[http://uaf-10.t2.ucsd.edu/~kdownham/WWZ/BDT_Information/v1/weights/Opposite_Flavor/][opposite flavor]] and [[http://uaf-10.t2.ucsd.edu/~kdownham/WWZ/BDT_Information/v1/weights/Same_Flavor/][same flavor]] BDTs * Plots will be shown [[http://uaf-10.t2.ucsd.edu/~kdownham/WWZ/BDT_Information/v1/plots/][here]] (WIP) ---+++ Training Region (TR) Selection Events passed to the BDT for training and testing are subject to the so-called "training region" selection, which is a subset of the full cut-based selection. A slide showing the training region selection can be found below: * Training region selection (v1): [[http://uaf-10.t2.ucsd.edu/~kdownham/WWZ/BDT_Information/v1/presentations/WWZ_BDT_Summary_092623.pdf][here]] (slide 3) ---
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Topic revision: r47 - 18 Jan 2024 - 03:44:28 -
KeeganDownham
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