pith. machine review for the scientific record. sign in

arxiv: 2605.13649 · v1 · submitted 2026-05-13 · ✦ hep-ex

Recognition: 2 theorem links

· Lean Theorem

Search for single vector-like quark production in opposite-sign dilepton final states in proton-proton collisions at sqrt{s} = 13 TeV

Authors on Pith no claims yet

Pith reviewed 2026-05-14 17:55 UTC · model grok-4.3

classification ✦ hep-ex
keywords vector-like top quarksingle productionT to tHopposite-sign dileptonsCMSLHCupper limits13 TeV
0
0 comments X

The pith

No excess observed in search for single vector-like top quark T decaying to top and Higgs in opposite-sign dilepton events.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper presents a search for single production of a vector-like top quark T decaying to a standard model top quark and Higgs boson. It analyzes proton-proton collision data at 13 TeV collected by CMS in 2016-2018, corresponding to up to 138 fb^{-1}, in a final state with two opposite-sign leptons, jets, and missing transverse momentum. No excess above expected background is found. Upper limits at 95% confidence level are set on the product of the T production cross section and branching fraction to tH, ranging from 2.0 pb at 600 GeV to 0.1 pb at 1000 GeV. This constitutes the first search in the T to tH channel using the opposite-sign dilepton final state.

Core claim

The analysis of 13 TeV proton-proton collision data in opposite-sign dilepton final states finds no excess over standard model background expectations for single production of a vector-like top quark T decaying to tH, resulting in 95% CL upper limits on the cross section times branching fraction from 2.0 pb at 600 GeV to 0.1 pb at 1000 GeV.

What carries the argument

Event selection requiring two opposite-sign leptons, multiple jets, and missing transverse momentum to isolate potential T to tH signals from background.

If this is right

  • Vector-like quark models predicting cross sections times branching fractions above the observed limits for T masses between 600 and 1000 GeV are excluded at 95% confidence level.
  • These results provide the first constraints specifically from the opposite-sign dilepton channel in the T to tH decay mode.
  • The limits can be combined with other searches in different final states to further restrict the allowed parameter space for vector-like top quarks.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • Future LHC data with higher luminosity could extend the mass reach or tighten the limits by a factor of several.
  • Complementary searches in single-lepton or fully hadronic channels would add sensitivity to the same T to tH signature.
  • These bounds can inform model-building efforts that incorporate vector-like quarks to address issues like the Higgs mass or flavor anomalies.

Load-bearing premise

Standard model backgrounds are accurately modeled in simulation with no significant unaccounted contributions, and signal efficiencies are correctly estimated for the assumed masses and decays.

What would settle it

Observing a statistically significant excess of events in the signal region beyond the predicted background would indicate the presence of the T quark signal.

Figures

Figures reproduced from arXiv: 2605.13649 by CMS Collaboration.

Figure 1
Figure 1. Figure 1: Leading-order Feynman diagram for the single production of a vector-like T quark [PITH_FULL_IMAGE:figures/full_fig_p003_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: Distributions of the reconstructed invariant mass in simulated signal events for T [PITH_FULL_IMAGE:figures/full_fig_p008_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: Comparison of the observed data and simulated background distributions of the [PITH_FULL_IMAGE:figures/full_fig_p011_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: Distribution of the reconstructed mass mtH in the background simulation, taking the channels ee (upper left), µµ (upper right), and eµ (lower) for the 2018 data, as an example. Superimposed as solid lines are the fits to the background model given by the function f0 in Eq. (2). The lower panels show the ratio of the MC distribution to the background function fit [PITH_FULL_IMAGE:figures/full_fig_p012_4.png] view at source ↗
Figure 5
Figure 5. Figure 5: Distributions of the invariant mass mtH in the ee (upper left), µµ (upper right), and eµ (lower) channels in 2016–2018 data set. In the upper panel, the black points show the data in the signal region, and the shapes from the background-only fits are in green. Expected signal distributions for three representative signal mass values are also shown, normalized to a cross section of 1 pb. The lower panel sho… view at source ↗
Figure 6
Figure 6. Figure 6: Expected and observed upper limits at 95% CL on the production cross section [PITH_FULL_IMAGE:figures/full_fig_p016_6.png] view at source ↗
Figure 7
Figure 7. Figure 7: Expected and observed upper limits at 95% CL on the production cross section [PITH_FULL_IMAGE:figures/full_fig_p017_7.png] view at source ↗
read the original abstract

A search is presented for single production of a vector-like top quark T, decaying into the standard model top quark and Higgs boson, in a final state including two opposite-sign leptons (electrons or muons), jets, and missing transverse momentum. The data were recorded by the CMS experiment in proton-proton collisions at a center-of-mass energy of 13 TeV at the CERN LHC in the years 2016$-$2018, and corresponding to an integrated luminosity of up to 138 fb$^{-1}$. No excess in data over the background expectations is observed. Upper limits at 95% confidence level on the product of the T production cross section and its decay branching fraction to tH are set, ranging from 2.0 pb at a T mass of 600 GeV to 0.1 pb at 1000 GeV. This is the first search in the T $\to$ tH channel in opposite-sign dilepton final states.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

0 major / 3 minor

Summary. The manuscript reports a search for single production of a vector-like top quark T decaying to tH in the opposite-sign dilepton final state (electrons or muons, jets, and missing transverse momentum). Using up to 138 fb^{-1} of CMS data at √s = 13 TeV from 2016–2018, no excess over background expectations is observed. 95% CL upper limits are set on σ(T) × BR(T → tH), ranging from 2.0 pb at m_T = 600 GeV to 0.1 pb at 1000 GeV. The work claims to be the first search in the T → tH channel using this final state.

Significance. If the background modeling and signal efficiencies hold, the result provides the first constraints on single T production in the opposite-sign dilepton tH channel, complementing existing VLQ searches in other final states and decay modes. The null-result limit-setting procedure follows established collider methods and adds a new, independent exclusion region.

minor comments (3)
  1. [Abstract and Section 3] The abstract states 'up to 138 fb^{-1}'; the main text should explicitly tabulate the luminosity used for each mass hypothesis and confirm that the same dataset is applied uniformly across the signal regions.
  2. [Background estimation] The description of the fake-lepton background estimation (Section 4 or equivalent) relies on data-driven methods; additional validation plots comparing the control regions to data would strengthen the claim that this contribution is accurately modeled in the signal region.
  3. [Results] Table or figure presenting the observed limits should include the expected limits and ±1σ/±2σ bands for direct visual comparison, as is standard for such searches.

Simulated Author's Rebuttal

0 responses · 0 unresolved

We thank the referee for their positive assessment of the manuscript, including the recognition that this search provides the first constraints on single T production in the opposite-sign dilepton tH channel. We appreciate the recommendation for minor revision. No specific major comments were raised in the report.

Axiom & Free-Parameter Ledger

0 free parameters · 2 axioms · 0 invented entities

The analysis rests on standard domain assumptions in high-energy physics rather than new free parameters or entities introduced in this work.

axioms (2)
  • domain assumption Standard Model background processes are well-understood and can be simulated accurately in the selected kinematic region.
    Essential for interpreting no excess as a constraint on new physics.
  • domain assumption Detector response, reconstruction efficiencies, and acceptances are correctly modeled in simulation for both signal and background.
    Required to compute signal efficiencies and expected backgrounds.

pith-pipeline@v0.9.0 · 5473 in / 1243 out tokens · 113556 ms · 2026-05-14T17:55:08.959516+00:00 · methodology

discussion (0)

Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.

Lean theorems connected to this paper

Citations machine-checked in the Pith Canon. Every link opens the source theorem in the public Lean library.

What do these tags mean?
matches
The paper's claim is directly supported by a theorem in the formal canon.
supports
The theorem supports part of the paper's argument, but the paper may add assumptions or extra steps.
extends
The paper goes beyond the formal theorem; the theorem is a base layer rather than the whole result.
uses
The paper appears to rely on the theorem as machinery.
contradicts
The paper's claim conflicts with a theorem or certificate in the canon.
unclear
Pith found a possible connection, but the passage is too broad, indirect, or ambiguous to say the theorem truly supports the claim.

Reference graph

Works this paper leans on

57 extracted references · 57 canonical work pages · 25 internal anchors

  1. [1]

    Sealing the fate of a fourth generation of fermions

    A. Djouadi and A. Lenz, “Sealing the fate of a fourth generation of fermions”,Phys. Lett. B715(2012) 310,doi:10.1016/j.physletb.2012.07.060,arXiv:1204.1252

  2. [2]

    Constraints on a fourth generation of fermions from Higgs boson searches

    A. Lenz, “Constraints on a fourth generation of fermions from Higgs boson searches”, Adv. High Energy Phys.2013(2013) 910275,doi:10.1155/2013/910275

  3. [3]

    Addressing the CKM unitarity problem with a vector-like up quark

    G. C. Branco et al., “Addressing the CKM unitarity problem with a vector-like up quark”,JHEP07(2021) 099,doi:10.1007/JHEP07(2021)099,arXiv:2103.13409

  4. [4]

    Cabibbo angle anomalies and oblique corrections: The remarkable role of the vectorlike quark doublet

    B. Belfatto and S. Trifinopoulos, “Cabibbo angle anomalies and oblique corrections: The remarkable role of the vectorlike quark doublet”,Phys. Rev. D108(2023) 035022, doi:10.1103/PhysRevD.108.035022,arXiv:2302.14097

  5. [5]

    Precise Measurement of the Pi+ -> Pi0 e+ nu Branching Ratio

    D. Pocanic et al., “Precise measurement of theπ + →π 0e+νbranching ratio”,Phys. Rev. Lett.93(2004) 181803,doi:10.1103/PhysRevLett.93.181803, arXiv:hep-ex/0312030. 18

  6. [6]

    Pion beta decay and Cabibbo-Kobayashi-Maskawa unitarity

    A. Czarnecki, W. J. Marciano, and A. Sirlin, “Pion beta decay and Cabibbo-Kobayashi-Maskawa unitarity”,Phys. Rev. D101(2020) 091301, doi:10.1103/PhysRevD.101.091301,arXiv:1911.04685

  7. [7]

    A handbook of vector-like quarks: mixing and single production

    J. A. Aguilar-Saavedra, R. Benbrik, S. Heinemeyer, and M. P ´erez-Victoria, “Handbook of vectorlike quarks: Mixing and single production”,Phys. Rev. D88(2013) 094010, doi:10.1103/PhysRevD.88.094010,arXiv:1306.0572

  8. [8]

    Combination of searches for singly produced vectorlike top quarks in pp collisions at √s=13 TeV with the ATLAS detector

    ATLAS Collaboration, “Combination of searches for singly produced vectorlike top quarks in pp collisions at √s=13 TeV with the ATLAS detector”,Phys. Rev. D111 (2025) 012012,doi:10.1103/PhysRevD.111.012012,arXiv:2408.08789

  9. [9]

    Review of searches for vector-like quarks, vector-like leptons, and heavy neutral leptons in proton–proton collisions at √s=13 TeV at the CMS experiment

    CMS Collaboration, “Review of searches for vector-like quarks, vector-like leptons, and heavy neutral leptons in proton–proton collisions at √s=13 TeV at the CMS experiment”,Phys. Rept.1115(2025) 570,doi:10.1016/j.physrep.2024.09.012, arXiv:2405.17605

  10. [10]

    Identifying top partners at LHC

    J. A. Aguilar-Saavedra, “Identifying top partners at LHC”,JHEP11(2009) 030, doi:10.1088/1126-6708/2009/11/030,arXiv:0907.3155

  11. [11]

    Search for electroweak production of a vector-like T quark using fully hadronic final states

    CMS Collaboration, “Search for electroweak production of a vector-like T quark using fully hadronic final states”,JHEP01(2020) 036,doi:10.1007/JHEP01(2020)036, arXiv:1909.04721

  12. [12]

    Search for a vector-like quark T ′→tH via the diphoton decay mode of the Higgs boson in proton-proton collisions at √s= 13 TeV

    CMS Collaboration, “Search for a vector-like quark T ′→tH via the diphoton decay mode of the Higgs boson in proton-proton collisions at √s= 13 TeV”,JHEP09(2023) 057, doi:10.1007/JHEP09(2023)057,arXiv:2302.12802

  13. [13]

    Search for production of a single vector-like quark decaying to tH or tZ in the all-hadronic final state in pp collisions at √s=13 TeV

    CMS Collaboration, “Search for production of a single vector-like quark decaying to tH or tZ in the all-hadronic final state in pp collisions at √s=13 TeV”,Phys. Rev. D110 (2024) 072012,doi:10.1103/PhysRevD.110.072012,arXiv:2405.05071

  14. [14]

    HEPData record for this analysis, 2026.doi:10.17182/hepdata.166760

  15. [15]

    The CMS experiment at the CERN LHC

    CMS Collaboration, “The CMS experiment at the CERN LHC”,JINST3(2008) S08004, doi:10.1088/1748-0221/3/08/S08004

  16. [16]

    Development of the CMS detector for the CERN LHC Run 3

    CMS Collaboration, “Development of the CMS detector for the CERN LHC Run 3”, JINST19(2024) P05064,doi:10.1088/1748-0221/19/05/P05064, arXiv:2309.05466

  17. [17]

    The CMS trigger system

    CMS Collaboration, “The CMS trigger system”,JINST12(2017) P01020, doi:10.1088/1748-0221/12/01/P01020,arXiv:1609.02366

  18. [18]

    Performance of the CMS Level-1 trigger in proton-proton collisions at √s=13 TeV

    CMS Collaboration, “Performance of the CMS Level-1 trigger in proton-proton collisions at √s=13 TeV”,JINST15(2020) P10017, doi:10.1088/1748-0221/15/10/P10017,arXiv:2006.10165

  19. [19]

    Performance of the CMS high-level trigger during LHC Run 2

    CMS Collaboration, “Performance of the CMS high-level trigger during LHC Run 2”, JINST19(2024) P11021,doi:10.1088/1748-0221/19/11/P11021, arXiv:2410.17038

  20. [20]

    Particle-flow reconstruction and global event description with the CMS detector

    CMS Collaboration, “Particle-flow reconstruction and global event description with the CMS detector”,JINST12(2017) P10003,doi:10.1088/1748-0221/12/10/P10003, arXiv:1706.04965. References 19

  21. [21]

    Technical proposal for the Phase-II upgrade of the Compact Muon Solenoid

    CMS Collaboration, “Technical proposal for the Phase-II upgrade of the Compact Muon Solenoid”, CMS Technical Proposal CERN-LHCC-2015-010, CMS-TDR-15-02, 2015

  22. [22]

    The anti-k_t jet clustering algorithm

    M. Cacciari, G. P . Salam, and G. Soyez, “The anti-kT jet clustering algorithm”,JHEP04 (2008) 063,doi:10.1088/1126-6708/2008/04/063,arXiv:0802.1189

  23. [23]

    FastJet user manual

    M. Cacciari, G. P . Salam, and G. Soyez, “Fastjet user manual”,Eur. Phys. J. C72(2012) 1896,doi:10.1140/epjc/s10052-012-1896-2,arXiv:1111.6097

  24. [24]

    Jet energy scale and resolution in the CMS experiment in pp collisions at 8 TeV

    CMS Collaboration, “Jet energy scale and resolution in the CMS experiment in pp collisions at 8 TeV”,JINST12(2017) P02014, doi:10.1088/1748-0221/12/02/P02014,arXiv:1607.03663

  25. [25]

    Pileup mitigation at CMS in 13 TeV data

    CMS Collaboration, “Pileup mitigation at CMS in 13 TeV data”,JINST15(2020) P09018, doi:10.1088/1748-0221/15/09/P09018,arXiv:2003.00503

  26. [26]

    Performance of missing transverse momentum reconstruction in proton-proton collisions at $\sqrt{s} =$ 13 TeV using the CMS detector

    CMS Collaboration, “Performance of missing transverse momentum reconstruction in proton-proton collisions at √s=13 TeV using the CMS detector”,JINST14(2019) P07004,doi:10.1088/1748-0221/14/07/P07004,arXiv:1903.06078

  27. [27]

    Jet flavour classification using DeepJet

    E. Bols et al., “Jet flavour classification usingDEEPJET”,JINST15(2020) P12012, doi:10.1088/1748-0221/15/12/P12012,arXiv:2008.10519

  28. [28]

    Performance summary of AK4 jet b tagging with data from proton-proton collisions at 13 TeV with the CMS detector

    CMS Collaboration, “Performance summary of AK4 jet b tagging with data from proton-proton collisions at 13 TeV with the CMS detector”, CMS Detector Performance Summary CMS-DP-2023-005, 2023

  29. [29]

    Identification of heavy-flavour jets with the CMS detector in pp collisions at 13 TeV

    CMS Collaboration, “Identification of heavy-flavour jets with the CMS detector in pp collisions at 13 TeV”,JINST13(2018) P05011, doi:10.1088/1748-0221/13/05/P05011,arXiv:1712.07158

  30. [30]

    Performance of theDEEPJETb tagging algorithm using 41.9 fb −1 of data from proton-proton collisions at 13 TeV with Phase 1 CMS detector

    CMS Collaboration, “Performance of theDEEPJETb tagging algorithm using 41.9 fb −1 of data from proton-proton collisions at 13 TeV with Phase 1 CMS detector”, CMS Detector Performance Summary CMS-DP-2018-058, 2018

  31. [31]

    The automated computation of tree-level and next-to-leading order differential cross sections, and their matching to parton shower simulations

    J. Alwall et al., “The automated computation of tree-level and next-to-leading order differential cross sections, and their matching to parton shower simulations”,JHEP07 (2014) 079,doi:10.1007/JHEP07(2014)079,arXiv:1405.0301

  32. [32]

    A general framework for implementing NLO calculations in shower Monte Carlo programs: the POWHEG BOX

    S. Alioli, P . Nason, C. Oleari, and E. Re, “A general framework for implementing NLO calculations in shower Monte Carlo programs: the POWHEG BOX”,JHEP06(2010) 043, doi:10.1007/JHEP06(2010)043,arXiv:1002.2581

  33. [33]

    Matching NLO QCD computations and parton shower simulations

    S. Frixione and B. R. Webber, “Matching NLO QCD computations and parton shower simulations”,JHEP06(2002) 029,doi:10.1088/1126-6708/2002/06/029, arXiv:hep-ph/0204244

  34. [34]

    Parton distributions from high-precision collider data

    NNPDF Collaboration, “Parton distributions from high-precision collider data”,Eur. Phys. J. C77(2017) 663,doi:10.1140/epjc/s10052-017-5199-5, arXiv:1706.00428

  35. [35]

    An Introduction to PYTHIA 8.2

    T. Sj ¨ostrand et al., “An introduction toPYTHIA8.2”,Comput. Phys. Commun.191(2015) 159,doi:10.1016/j.cpc.2015.01.024,arXiv:1410.3012. 20

  36. [36]

    GEANT4 — a simulation toolkit

    GEANT4 Collaboration, “GEANT4— a simulation toolkit”,Nucl. Instrum. Meth. A506 (2003) 250,doi:10.1016/S0168-9002(03)01368-8

  37. [37]

    Electron and photon reconstruction and identification with the CMS experiment at the CERN LHC

    CMS Collaboration, “Electron and photon reconstruction and identification with the CMS experiment at the CERN LHC”,JINST16(2021) P05014, doi:10.1088/1748-0221/16/05/P05014,arXiv:2012.06888

  38. [38]

    Performance of the CMS muon detector and muon reconstruction with proton-proton collisions at $\sqrt{s}=$ 13 TeV

    CMS Collaboration, “Performance of the CMS muon detector and muon reconstruction with proton-proton collisions at √s=13 TeV”,JINST13(2018) P06015, doi:10.1088/1748-0221/13/06/P06015,arXiv:1804.04528

  39. [39]

    CMS jet algorithms performance in 13 TeV data

    CMS Collaboration, “CMS jet algorithms performance in 13 TeV data”, CMS Physics Analysis Summary CMS-PAS-JME-16-003, 2017

  40. [40]

    Navaset al.[Particle Data Group], Phys

    Particle Data Group Collaboration, “Review of particle physics”,Phys. Rev. D110(2024) 030001,doi:10.1103/PhysRevD.110.030001

  41. [41]

    Search for heavy resonances decaying to a pair of lorentz-boosted higgs bosons in final states with leptons and a bottom quark pair at √s=13 TeV

    CMS Collaboration, “Search for heavy resonances decaying to a pair of lorentz-boosted higgs bosons in final states with leptons and a bottom quark pair at √s=13 TeV”,JHEP 05(2022) 005,doi:10.1007/JHEP05(2022)005,arXiv:2112.03161

  42. [42]

    A study of the reactionsψ ′ →γγψ

    M. J. Oreglia, “A study of the reactionsψ ′ →γγψ”. PhD thesis, Stanford University,

  43. [43]

    SLAC Report SLAC-R-236, see Appendix D

  44. [44]

    Charmonium spectroscopy from radiative decays of theJ/ψandψ ′

    J. E. Gaiser, “Charmonium spectroscopy from radiative decays of theJ/ψandψ ′”. PhD thesis, Stanford University, 1982. SLAC Report SLAC-R-255

  45. [45]

    Sensitivity of searches for new signals and its optimization

    G. Punzi, “Sensitivity of searches for new signals and its optimization”, p. MODT002. 2003.arXiv:physics/0308063. econf C030908

  46. [46]

    Handling uncertainties in background shapes: the discrete profiling method

    P . D. Dauncey, M. Kenzie, N. Wardle, and G. J. Davies, “Handling uncertainties in background shapes: the discrete profiling method”,JINST10(2015) P04015, doi:10.1088/1748-0221/10/04/P04015,arXiv:1408.6865

  47. [47]

    Precision luminosity measurement in proton-proton collisions at√s=13 TeV in 2015 and 2016 at CMS

    CMS Collaboration, “Precision luminosity measurement in proton-proton collisions at√s=13 TeV in 2015 and 2016 at CMS”,Eur. Phys. J. C81(2021) 800, doi:10.1140/epjc/s10052-021-09538-2,arXiv:2104.01927

  48. [48]

    CMS luminosity measurement for the 2017 data-taking period at√s= 13 TeV

    CMS Collaboration, “CMS luminosity measurement for the 2017 data-taking period at√s= 13 TeV”, CMS Physics Analysis Summary CMS-PAS-LUM-17-004, 2018

  49. [49]

    CMS luminosity measurement for the 2018 data-taking period at√s= 13 TeV

    CMS Collaboration, “CMS luminosity measurement for the 2018 data-taking period at√s= 13 TeV”, CMS Physics Analysis Summary CMS-PAS-LUM-18-002, 2019

  50. [50]

    Measurement of the Inclusive W and Z Production Cross Sections in pp Collisions at sqrt(s) = 7 TeV

    CMS Collaboration, “Measurement of the W and Z inclusive production cross sections at√s=7 TeV with the CMS experiment at the LHC”,JHEP10(2011) 132, doi:10.1007/JHEP10(2011)132,arXiv:1107.4789

  51. [51]

    Measurement of the inelastic proton-proton cross section at $\sqrt{s}=$ 13 TeV

    CMS Collaboration, “Measurement of the inelastic proton-proton cross section at √s=13 TeV”,JHEP07(2018) 161,doi:10.1007/JHEP07(2018)161,arXiv:1802.02613

  52. [52]

    Performance of the CMS electromagnetic calorimeter in pp collisions at √s=13 TeV

    CMS Collaboration, “Performance of the CMS electromagnetic calorimeter in pp collisions at √s=13 TeV”,JINST19(2024) P09004, doi:10.1088/1748-0221/19/09/P09004,arXiv:2403.15518. References 21

  53. [53]

    PDF4LHC recommendations for LHC Run II

    J. Butterworth et al., “PDF4LHC recommendations for LHC Run II”,J. Phys. G43(2016) 023001,doi:10.1088/0954-3899/43/2/023001,arXiv:1510.03865

  54. [54]

    Confidence Level Computation for Combining Searches with Small Statistics

    T. Junk, “Confidence level computation for combining searches with small statistics”, Nucl. Instrum. Meth. A434(1999) 435,doi:10.1016/S0168-9002(99)00498-2, arXiv:hep-ex/9902006

  55. [55]

    Presentation of search results: the CL s technique

    A. L. Read, “Presentation of search results: TheCL s technique”,J. Phys. G28(2002) 2693, doi:10.1088/0954-3899/28/10/313

  56. [56]

    Asymptotic formulae for likelihood-based tests of new physics

    G. Cowan, K. Cranmer, E. Gross, and O. Vitells, “Asymptotic formulae for likelihood-based tests of new physics”,Eur. Phys. J. C71(2011) 1554, doi:10.1140/epjc/s10052-011-1554-0,arXiv:1007.1727. [Erratum: doi:10.1140/epjc/s10052-013-2501-z]

  57. [57]

    Vector-like Fermions and Higgs Effective Field Theory Revisited

    C.-Y. Chen, S. Dawson, and E. Furlan, “Vectorlike fermions and Higgs effective field theory revisited”,Phys. Rev. D96(2017) 015006, doi:10.1103/PhysRevD.96.015006,arXiv:1703.06134. 22 23 A The CMS Collaboration Yerevan Physics Institute, Yerevan, Armenia A. Hayrapetyan, V . Makarenko , A. Tumasyan1 Institut f ¨ ur Hochenergiephysik, Vienna, Austria W. Ada...