searches for new physics with unconventional signatures
play

Searches for new physics with unconventional signatures at ATLAS - PowerPoint PPT Presentation

FERMILAB-SLIDES-19-013-PPD Searches for new physics with unconventional signatures at ATLAS and CMS Kevin Pedro (FNAL) on behalf of the ATLAS and CMS Collaborations March 26, 2019 This document was prepared by [ATLAS AND CMS Collabrations]


  1. FERMILAB-SLIDES-19-013-PPD Searches for new physics with unconventional signatures at ATLAS and CMS Kevin Pedro (FNAL) on behalf of the ATLAS and CMS Collaborations March 26, 2019 This document was prepared by [ATLAS AND CMS Collabrations] using the resources of the Fermi National Accelerator Laboratory (Fermilab), a U.S. Department of Energy, Office of Science, HEP User Facility. Fermilab is managed by Fermi Research Alliance, LLC (FRA), acting under Contract No. DE-AC02-07CH11359.

  2. Unconventional Models • Hidden sector : new particles & forces • Small coupling to SM → long lifetime • Unusual dynamics or striking signatures [M. Lisanti] [Claire David] • Supersymmetry : superpartner for each SM particle w/ ½ spin difference • R-parity violating, split, stealth, gauge- or anomaly-mediated SUSY breaking… • Long lifetimes tend to occur in compressed scenarios (near- degenerate masses) or with suppressed decays Moriond QCD 2019 Kevin Pedro 2

  3. Challenges [xkcd] Reconstruction : • “Standard” methods optimized for prompt decays → may fail for long-lived particles • Need to rely on missing energy or ionization to detect ~stable BSM particles • Hard to trigger on many unconventional signatures  Rely on low-level subdetector information Backgrounds : • Mostly instrumental or other unusual sources • Probably not simulated well (if at all) • SM has LLPs, e.g. B hadrons  Need data-driven methods Moriond QCD 2019 Kevin Pedro 3

  4. neutral BSM emerging HSCP charged lepton jet any charge quark photon [J. Antonelli] anything displaced disappearing lepton track displaced displaced photon dijet Not pictured: displaced displaced out of time decays vertex conversion 4

  5. Search for Emerging Jets • Dark QCD force w/ dark quarks → form dark mesons & baryons • These decay after non-negligible lifetime to SM hadrons → emerging jets • Tag emerging jets using track impact parameter variables • Require 4 jets w/ 2 tagged emerging jets (or 1 tagged and miss > 200 GeV for large cτ), trigger on H T = ∑p T (j 1,2,3,4 ) p T • Combine tagging WPs w/ kinematic selections → 7 signal regions • Background: misid. rate (from γ CR) × QCD CR yield = SR yield (cτ = 25 mm) (2D) › / 1cm) log(‹d 0 Moriond QCD 2019 Kevin Pedro 5

  6. Emerging Jet Results • Data: 16.1 fb -1 , √s = 13 TeV, 2016 • JHEP02(2019)179, arXiv:1810.10069 • Observed data agree with background predictions (within uncertainties ) • Limits do not depend strongly on m πd  Exclude m Xd between 400 and 1250 GeV for cτ πd between 5 and 225 mm (Signal yields in table shown for largest m Xd excluded by each selection set) Moriond QCD 2019 Kevin Pedro 6

  7. Search for Heavy Charged LLPs • R-hadrons : bound state of SUSY & SM colored particles New! o Gluinos (split SUSY) or stops (electroweak baryogenesis)  Use “full-detector” or “MS-agnostic” (no muon spectrometer) • Electroweak SUSY : staus (GMSB) or charginos (AMSB)  Use both inner detector (ID) and muon spectrometer (MS) miss • Trigger on single muon or p T  Measure candidate velocity (β) and mass (m = p/βγ) from dE/dx or ToF • Background: sample mass values from distrs. of p, β ToF , (βγ) dE/dx Moriond QCD 2019 Kevin Pedro 7

  8. Heavy Charged LLP Results • Data: 36.1 fb -1 , New! √s = 13 TeV, 2015/16 • arXiv:1902.01636 • No significant excess m g̃ < 1.86–1.98 TeV observed m g̃ < 2.0 TeV • Limits degrade slightly for meta-stable R-hadrons m χ̃± 1 < 1.09 TeV m τ̃ < 430 GeV m t̃ < 1.34 TeV Moriond QCD 2019 Kevin Pedro 8

  9. Search for Delayed Jets • GMSB SUSY w/ long-lived gluinos Run 2! miss → R-hadrons decay to delayed jets + p T • First use of ECAL timing to distinguish displaced jets: t jet = median(t cell ), ΔR(cell, jet) < 0.4, t cell < 20 ns miss (w/ out-of-time ECAL) • Calorimeter jets and p T • Cathode Strip Chambers (CSC) & HCAL reject beam halo • Tracks reject satellite bunches & mismeasurements • Drift Tubes (DT) and Resistive Plate Chambers (RPC) reject cosmics • ECAL rejects pileup & APD hits • Backgrounds : invert cleaning cuts to form data CRs Normalized CR templates Signal region: N jet ≥ 1, t jet > 3 ns Moriond QCD 2019 Kevin Pedro 9

  10. Delayed Jet Results • Data: 137.4 fb -1 , √s = 13 TeV, full Run 2! (2016/2017/2018) Run 2! + 2.5 • Observed: 0 events, in agreement w/ background prediction: 1 – 1  Exclude m g̃ < 2.5 TeV for cτ 0 ~ 1 m or m g̃ < 2.0 TeV for cτ 0 ~ 10 m • Significantly extends reach for cτ 0 ≥ 1 m (vs. tracker-based searches) • CMS-PAS-EXO-19-001 Moriond QCD 2019 Kevin Pedro 10

  11. Search for Displaced Hadronic Jets • Simplified hidden sector, Φ → s s → f ¯ f f′ ¯ f′ New! • Custom triggers using CalRatio = E HCAL /E ECAL o High-E T and low-E T versions (33.0 fb -1 or 10.8 fb -1 , √s = 13 TeV, 2016) o Separate data streams for cosmic and beam- induced background (BIB)  MLP predicts jet decay position ↴  Jet BDT classifies jets: signal, QCD, or BIB ↴  Event BDTs optimized for high-E T and low-E T • Multijet background: o Use ∑ΔR min (jets,trk) and event BDT score o Simultaneous fit to signal and background • arXiv:1902.03094 Moriond QCD 2019 Kevin Pedro 11

  12. SUSY w/ Disappearing Tracks • Data: 137.4 fb -1 , √s = 13 TeV, full Run 2! (2016/2017/2018) Run 2! • Compressed SUSY w/ Δm(χ̃ ± 1 ,χ̃ 0 1 ) ~ 100 MeV, cτ(χ̃ ± 1 ) ~ 50 cm • Require ≥2 jets, M T2 > 200 GeV, at least one short track (ST) • Bin in N jet , H T , ST length, ST p T : 68 search regions • Background: fake rate applied to ST “candidates” (relaxed quality, isolation req.) • Exclude m g̃ < 2.46 TeV and m χ̃0 1 < 2.0 TeV  Improvement of 210 GeV and 525 GeV (resp.) in compressed region • CMS-PAS-SUS-19-005 Moriond QCD 2019 Kevin Pedro 12

  13. Search for Displaced Vertex & Muon • R-parity violating SUSY w/ t̃ as LSP and small Run 2! λ′ 23k coupling → suppressed decays, R-hadrons • Large-radius tracking (LRT) improves efficiency for tracks with large impact parameters • Displaced vertices (DV) reconstructed w/ secondary vertex algorithm • Muon spectrometer rejects cosmic background and fake muons • Inner detector rejects heavy flavor • Backgrounds: transfer factors from DV CRs applied to muon CRs (in data) • Signal regions from triggers: miss > 180 GeV o p T μ > 60 GeV, |η| < 2.5 o p T miss < 180 GeV) (p T Moriond QCD 2019 Kevin Pedro 13

  14. Displaced Vertex & Muon Results • Data: 136 fb -1 , √s = 13 TeV, full Run 2! (2016/2017/2018) Run 2! • ATLAS-CONF-2019-006 Predicted Obs. • Exclude m t̃ < 1.7 TeV for τ t̃ = 0.1 ns miss Trigger SR p T 0.43 ± 0.16 ± 0.16 0 ( m t̃ < 1.3 TeV for 0.01 < τ t̃ < 30 ns ) μ Trigger SR 1.88 ± 0.20 ± 0.28 1  Strictest limits to date for metastable t̃ decaying via λ′ ijk • Model-independent limits on # signal events and σ vis also derived Moriond QCD 2019 Kevin Pedro 14

  15. Conclusions • Growing interest in searches for new physics with unconventional signatures • Presented today: emerging jets, heavy charged LLPs, delayed jets, displaced jets, disappearing tracks, displaced muons o Including full Run 2 results from both collaborations o Many other interesting analyses: CMS: EXO, SUS; ATLAS: EXOT, SUSY • Sensitive to decay lengths from 1 mm to 100+ m • Exclude new particles with masses up to ~1–2 TeV • New community white paper just released: “Searching for long-lived particles beyond the Standard Model at the Large Hadron Collider”, arXiv:1903.04497 Moriond QCD 2019 Kevin Pedro 15

  16. Backup

  17. ATLAS Summary https://atlas.web.cern.ch/Atlas/ GROUPS/PHYSICS/Combined SummaryPlots/EXOTICS/ https://atlas.web.cern.ch/Atlas/ GROUPS/PHYSICS/Combined SummaryPlots/SUSY/ Moriond QCD 2019 Kevin Pedro 17

  18. CMS Summary http://cms-results.web.cern.ch/cms- results/public- results/publications/EXO/index.html https://twiki.cern.ch/twiki/bin/view/CMSPublic/ SummaryPlotsEXO13TeV Moriond QCD 2019 Kevin Pedro 18

  19. Emerging Jet Details Tagging WPs Jet Selections • Each jet: Mis- o n trk ≥ 1 QCD control selections reco o p T (trk)/p T (j) < 0.6 Reject o f ch. EM < 0.9 ele. o f neu. EM < 0.9 Signal Regions • p T (j 1 ) > 225 GeV, p T (j 2,3,4 ) > 100 GeV Moriond QCD 2019 Kevin Pedro 19

  20. Emerging Jet Background  SM jets misidentified as emerging jets Photon CRs • Misid. rate (from γ CR) × QCD CR yield = SR yield • N γ = 1, p T > 175 GeV, |η| < 1.44 • Misid. rate higher for b quarks vs. light flavor • N SMJ ≥ 1, p T > 50 GeV, → get CR flavor compositions from CSVv2 dist. CSVv2 > 0.8 OR < 0.2 • Uncertainties: b quark fraction (0.6–5%), non-b quark miss > 200) QCD CRs composition (1.4–6.3%, 28.3% for p T miss > 200 • N EMJ = 0, p T miss ≥ 0 OR N EMJ = 1, p T QCD sideband Tagging WP 1 Selection set 1 Moriond QCD 2019 Kevin Pedro 20

Recommend


More recommend