[1] M. Czakon; P. Fiedler; A. Mitov The total top quark pair production cross-section at hadron colliders through $𝒪\left({\alpha }_S^4\right)$, Phys. Rev. Lett., Volume 110 (2013), 252004 | DOI

[2] LHCb Collaboration Measurement of forward top pair production in the dilepton channel in pp collisions at $\sqrt{s}=13$ TeV, JHEP, Volume 08 (2018), 174

[3] https://twiki.cern.ch/twiki/bin/view/LHCPhysics/LHCTopWG (LHCTopWG - LHC Top Physics Working Group)

[4] T. Jezo; J. M. Lindert; N. Moretti; S. Pozzorini New NLOPS predictions for $t\overline{t}+b$-jet production at the LHC, Eur. Phys. J. C, Volume 78 (2018), 502 | DOI

[5] ATLAS Collaboration Measurements of fiducial and differential cross-sections of $t\overline{t}$ production with additional heavy-flavour jets in proton–proton collisions at $\sqrt{s}=13$ TeV with the ATLAS detector, JHEP, Volume 04 (2019), 46 | DOI

[6] CMS Collaboration Measurements of $t\overline{t}$ cross sections in association with b jets and inclusive jets and their ratio using dilepton final states in pp collisions at $\sqrt{s}=13$ TeV, Phys. Lett. B, Volume 776 (2018), pp. 355-378

[7] (CMS Collaboration, “Measurement of the $t\overline{t}b\overline{b}$ production cross section in the all-jet final state in pp collisions at $\sqrt{s}=13$ TeV”, CMS Physics Analysis Summary, CMS-PAS-TOP-18-011)

[8] ATLAS Collaboration Evidence for single top-quark production in the s-channel in proton–proton collisions at $\sqrt{s}=8$ TeV with the ATLAS detector using the Matrix Element Method, Phys. Lett. B, Volume 756 (2016), pp. 228-246

[9] ATLAS and CMS Collaborations Combinations of single-top-quark production cross-section measurements and |f${}_{\mathrm{LV}}$ V${}_{\mathit{tb}}$| determinations at $\sqrt{s}=7$ and 8 TeV with the ATLAS and CMS experiments, JHEP, Volume 05 (2019), 88

[10] CMS Collaboration Measurement of the differential cross section for top quark pair production in pp collisions at $\sqrt{s}=8$ TeV, Eur. Phys. J. C, Volume 75 (2015), 542 | DOI

[11] ATLAS Collaboration Measurements of top-quark pair differential cross-sections in the lepton+jets channel in pp collisions at $\sqrt{s}=8$ TeV using the ATLAS detector, Eur. Phys. J. C, Volume 76 (2016), 538

[12] ATLAS Collaboration Measurements of top-quark pair differential cross-sections in the e$\mu$ channel in pp collisions at $\sqrt{s}=13$ TeV using the ATLAS detector, Eur. Phys. J. C, Volume 77 (2017), 299

[13] ATLAS Collaboration Measurements of differential cross sections of top quark pair production in association with jets in pp collisions at $\sqrt{s}=13$ TeV using the ATLAS detector, JHEP, Volume 10 (2018), 159 | DOI

[14] CMS Collaboration Measurement of differential cross sections for the production of top quark pairs and of additional jets in lepton+jets events from pp collisions at $\sqrt{s}=13$ TeV, Phys. Rev. D, Volume 97 (2018), 092005

[15] CMS Collaboration Measurements of $t\overline{t}$ differential cross sections in proton–proton collisions at $\sqrt{s}=13$ TeV using events containing two leptons, JHEP, Volume 02 (2019), 149

[16] ATLAS Collaboration Fiducial, total and differential cross-section measurements of t-channel single top-quark production in pp collisions at 8 TeV using data collected by the ATLAS detector, Eur. Phys. J. C, Volume 77 (2017), 531

[17] (CMS Collaboration, “Measurement of differential cross sections and charge ratios for t-channel single top quark production at 13 TeV”, CMS Physics Analysis Summary, CMS-PAS-TOP-17-023)

[18] CMS Collaboration Measurement of the integrated and differential $t\overline{t}$ production cross sections for high-p${}_{\mathrm{T}}$ top quarks in pp collisions at $\sqrt{s}=8$ TeV, Phys. Rev. D, Volume 94 (2016), 072002

[19] ATLAS Collaboration Measurement of the differential cross-section of highly boosted top quarks as a function of their transverse momentum in $\sqrt{s}=8$ TeV proton–proton collisions using the ATLAS detector, Phys. Rev. D, Volume 93 (2016), 032009

[20] ATLAS Collaboration Measurements of $t\overline{t}$ differential cross-sections of highly boosted top quarks decaying to all-hadronic final states in pp collisions at $\sqrt{s}=13$ TeV using the ATLAS detector, Phys. Rev. D, Volume 98 (2018), 012003

[21] ATLAS Collaboration Probing the quantum interference between singly and doubly resonant top-quark production in pp collisions at $\sqrt{s}=13$ TeV with the ATLAS detector, Phys. Rev. Lett., Volume 121 (2018), 152002

[22] CMS Collaboration Study of the underlying event in top quark pair production in pp collisions at 13 TeV, Eur. Phys. J. C, Volume 79 (2019), 123

[23] (CMS Collaboration, “Investigations of the impact of the parton shower tuning in Pythia 8 in the modelling of $t\overline{t}$ at $\sqrt{s}=8$ and 13 TeV”, CMS Physics Analysis Summary, CMS-PAS-TOP-16-021)

[24] CMS Collaboration Measurement of jet substructure observables in $t\overline{t}$ events from proton–proton collisions at $\sqrt{s}=13$ TeV, Phys. Rev. D, Volume 98 (2018), 092014

[25] CMS Collaboration Extraction and validation of a new set of CMS PYTHIA8 tunes from underlying-event measurements, Eur. Phys. J. C, Volume 80 (2020) no. 1, 4 | DOI

[26] ATLAS Collaboration Measurement of $K_S^0$ and ${\Lambda }_0$ production in $t\overline{t}$ dileptonic events in pp collisions at $\sqrt{s}=7$ TeV with the ATLAS detector, Eur. Phys. J. C, Volume 79 (2019) no. 12, 1017

[27] ATLAS Collaboration Measurement of jet shapes in top pair events at $\sqrt{s}=7$ TeV using the ATLAS detector, Eur. Phys. J. C, Volume 73 (2013), 2676

[28] CMS Collaboration Measurement of the top quark mass using charged particles in pp collisions at $\sqrt{s}=8$ TeV, Phys. Rev. D, Volume 93 (2016), 092006

[29] ATLAS Collaboration Measurement of colour flow using jet-pull observables in $t\overline{t}$ events with the ATLAS experiment at $\sqrt{s}=13$ TeV, Eur. Phys. J. C, Volume 78 (2018), 847

[30] M. Beneke; P. Marquard; P. Nason; M. Steinhauser On the ultimate uncertainty of the top quark pole mass, J. Phys. Lett. B, Volume 10 (2017), pp. 63-70 | DOI

[31] A. H. Hoang; C. Lepenik; M. Preisser On the light massive flavor dependence of the large order asymptotic behavior and the ambiguity of the pole mass, JHEP, Volume 09 (2017), 99 | DOI

[32] CMS Collaboration Measurement of the top quark mass using proton–proton data at $\sqrt{s}=7$ and 8 TeV, Phys. Rev. D, Volume 93 (2016), 072004

[33] ATLAS Collaboration Measurement of the top quark mass in the $t\overline{t}\to$ lepton+jets channel from $\sqrt{s}=8$ TeV ATLAS data and combination with previous results, Eur. Phys. J. C, Volume 79 (2019), 290

[34] (ATLAS Collaboration, “Measurement of the top quark mass using a leptonic invariant mass in pp collisions at $\sqrt{s}=13$ TeV with the ATLAS detector”, ATLAS-CONF-2019-046)

[35] S. F. Ravasio; T. Jazo; P. Nason; C. Oleari A theoretical study of top-mass measurements at the LHC using NLO+PS generators of increasing accuracy, Eur. Phys. J. C, Volume 78 (2018), 458

[36] G. Corcella; R. Franceschini; D. Kim Fragmentation uncertainties in hadronic observables for top quark mass measurements, Nucl. Phys. B, Volume 929 (2018), pp. 485-526 | DOI | MR | Zbl

[37] G. Heinrich; A. Maier; R. Nisius; J. Schlenk; M. Schulze; L. Scyboz; J. Winter NLO and off-shell effects in top quark mass determinations, JHEP, Volume 07 (2018), 129

[38] (CMS Collaboration, “Measurement of the jet mass distribution in highly boosted top quark decays in pp collisions at $\sqrt{s}=13$ TeV”, CMS Physics Analysis Summary, CMS-PAS-TOP-19-005)

[39] CMS Collaboration Measurement of the $t\overline{t}$ production cross section in the e$\mu$ channel in proton–proton collisions at $\sqrt{s}=7$ and 8 TeV, JHEP, Volume 08 (2016), 29

[40] ATLAS Collaboration Measurement of lepton differential distributions and the top quark mass in $t\overline{t}$ production in pp collisions at $\sqrt{s}=8$ TeV with the ATLAS detector, Eur. Phys. J. C, Volume 77 (2017), 804

[41] ATLAS Collaboration Measurement of the top-quark mass in $t\overline{t}+1$-jet events collected with the ATLAS detector in pp collisions at $\sqrt{s}=8$ TeV, JHEP, Volume 11 (2019), 150

[42] CMS Collaboration, “Measurement of $t\overline{t}$ normalised multi-differential cross sections in pp collisions at $\sqrt{s}=13$ TeV, and simultaneous determination of the strong coupling strength, top quark pole mass, and parton distribution functions”, Eur. Phys. J. C (2019) arXiv:1904.05237 (submitted)

[43] S. F. Ravasio; P. Nason; C. Oleari All-orders behaviour and renormalons in top-mass observables, 2019 (preprint) | arXiv

[44] M. Butenschoen Top quark mass calibration for Monte Carlo event generators, Phys. Rev. Lett., Volume 117 (2016), 232001 | DOI

[45] A. H. Hoang; S. Mantry; A. Pathak; I. W. Stewart Extracting a short distance top mass with light grooming, 2017 (preprint) | arXiv

[46] A. H. Hoang; S. Plätzer; D. Samitz On the cutoff dependence of the quark mass parameter in angular ordered parton showers, JHEP, Volume 10 (2018), 200

[47] CMS Collaboration Running of the top quark mass from proton–proton collisions at $\sqrt{s}=13$ TeV, Phys. Lett. B, Volume 803 (2020), 135263

[48] CMS Collaboration Measurement of the ratio $ℬ(t\to Wb)/ℬ(t\to Wq)$ in pp collisions at $\sqrt{s}=8$ TeV, Phys. Lett. B, Volume 736 (2014), pp. 33-57 | DOI

[49] (ATLAS Collaboration, “Measurement of the top-quark decay width in top-quark pair events in the dilepton channel at $\sqrt{s}=13$ TeV with the ATLAS detector”, ATLAS-CONF-2019-038)

[50] ATLAS Collaboration, “Measurements of top-quark pair spin correlations in the e$\mu$ channel at $\sqrt{s}=13$ TeV using pp collisions in the ATLAS detector”, Eur. Phys. J. C (2019) (submitted) | arXiv

[51] CMS Collaboration Measurement of the top quark polarization and $t\overline{t}$ spin correlations using dilepton final states in proton–proton collisions at $\sqrt{s}=13$ TeV, Phys. Rev. D, Volume 100 (2019) no. 7, 072002

[52] ATLAS Collaboration Measurements of top quark spin observables in $t\overline{t}$ events using dilepton final states in $\sqrt{s}=8$ TeV pp collisions with the ATLAS detector, JHEP, Volume 1703 (2017), 113

[53] (ATLAS Collaboration, “Inclusive and differential measurement of the charge asymmetry in $t\overline{t}$ events at 13 TeV with the ATLAS detector”, ATLAS-CONF-2019-026)

[54] CMS Collaboration Measurement of differential cross sections and charge ratios for t-channel single top quark production in proton–proton collisions at $\sqrt{s}=13$ TeV, Eur. Phys. J. C, Volume 80 (2020) no. 5, 370

[55] ATLAS and CMS Collaborations Combination of inclusive and differential $\mathrm{t}\overline{\mathrm{t}}$ charge asymmetry measurements using ATLAS and CMS data at $\sqrt{s}=7$ and 8 TeV, JHEP, Volume 04 (2018), 33

[56] HL-LHC Collaboration and HE-LHC Working Group Standard Model Physics at the HL-LHC and HE-LHC, 2019 (preprint) | arXiv

[57] ATLAS Collaboration Measurements of charge and CP asymmetries in b-hadron decays using top-quark events collected by the ATLAS detector in pp collisions at $\sqrt{s}=8$ TeV, JHEP, Volume 1702 (2017), 71

[58] ATLAS Collaboration Measurement of the W boson polarisation in $t\overline{t}$ events from pp collisions at $\sqrt{s}=8$ TeV in the lepton + jets channel with ATLAS, Eur. Phys. J. C, Volume 77 (2017), 264 Erratum: Eur. Phys. J. C 79 (2019)

[59] CMS Collaboration Measurement of the W boson helicity fractions in the decays of top quark pairs to lepton + jets final states produced in pp collisions at $\sqrt{s}=8$ TeV, Phys. Lett. B, Volume 762 (2016), pp. 512-534 | DOI

[60] B. Grzadkowski; M. Iskrzynski; M. Misiak; J. Rosiek Dimension-six terms in the standard model Lagrangian, JHEP, Volume 10 (2010), 85 | Zbl

[61] ATLAS Collaboration Measurement of the $t\overline{t}Z$ and $t\overline{t}W$ cross sections in proton–proton collisions at $\sqrt{s}=13$ TeV with the ATLAS detector, Phys. Rev. D, Volume 99 (2019), 072009

[62] CMS Collaboration Measurement of the cross section for top quark pair production in association with a W or Z boson in proton–proton collisions at $\sqrt{s}=13$ TeV, JHEP, Volume 08 (2018), 11

[63] CMS Collaboration Measurement of top quark pair production in association with a Z boson in proton–proton collisions at $\sqrt{s}=13$ TeV, JHEP, Volume 03 (2020), 56

[64] CMS Collaboration Evidence for the associated production of a single top quark and a photon in proton–proton collisions at $\sqrt{s}=13$ TeV, Phys. Rev. Lett., Volume 121 (2018), 221802

[65] CMS Collaboration Observation of single top quark production in association with a Z boson in proton–proton collisions at $\sqrt{s}=13$ TeV, Phys. Rev. Lett., Volume 122 (2019), 132003

[66] (ATLAS Collaboration, “Observation of the associated production of a top quark and a Z boson in pp collisions at $\sqrt{s}=13$ TeV with the ATLAS detector”, ATLAS-CONF-2019-043)

[67] (ATLAS Collaboration, “Measurements of inclusive and differential cross-sections of $t\overline{t}\gamma$ production in the e$\mu$ channel at 13 TeV with the ATLAS detector”, ATLAS-CONF-2019-042)

[68] ATLAS Collaboration Search for four-top-quark production in the single-lepton and opposite-sign dilepton final states in pp collisions at $\sqrt{s}=13$ TeV with the ATLAS detector, Phys. Rev. D, Volume 99 (2019), 052009

[69] CMS Collaboration Search for production of four top quarks in final states with same-sign or multiple leptons in proton–proton collisions at $\sqrt{s}=13$ TeV, Eur. Phys. J. C, Volume 80 (2020) no. 2, 75

[70] CMS Collaboration Search for the flavor-changing neutral current interactions of the top quark and the Higgs boson which decays into a pair of b quarks at $\sqrt{s}=13$ TeV, JHEP, Volume 06 (2018), 102

[71] ATLAS Collaboration Search for top-quark decays t $\to$ Hq with 36 fb${}^{-1}$ of pp collision data at $\sqrt{s}=13$ TeV with the ATLAS detector, JHEP, Volume 05 (2019), 123

[72] ATLAS Collaboration Search for flavor-changing neutral currents in top quark decays t $\to$ Hc and t $\to$ Hu in multilepton final states in proton–proton collisions at $\sqrt{s}=13$ TeV with the ATLAS detector, Phys. Rev. D, Volume 98 (2018), 032002

[73] ATLAS Collaboration Search for top quark decays t$\to$qH, with H $\to \gamma \gamma$, in $\sqrt{s}=13$ TeV pp collisions using the ATLAS detector, JHEP, Volume 10 (2017), 129

[74] ATLAS Collaboration Search for flavour-changing neutral currents in processes with one top quark and a photon using 81 fb${}^{-1}$ of pp collisions at $\sqrt{s}=13$ TeV with the ATLAS experiment, Phys. Lett. B, Volume 800 (2020), 135082

[75] ATLAS Collaboration Search for flavour-changing neutral current top-quark decays t $\to$ qZ in proton–proton collisions at $\sqrt{s}=13$ TeV with the ATLAS detector, JHEP, Volume 07 (2018), 176

[76] (CMS Collaboration, “Search for flavour changing neutral currents in top quark production and decays with three-lepton final state using the data collected at $\sqrt{s}=13$ TeV”, CMS Physics Analysis Summary, CMS-PAS-TOP-17-017)

[77] F. Simon A first look at the impact of NNNLO theory uncertainties on top mass measurements at the ILC, 2016 (preprint) | arXiv

[78] M. S. Amjad A precise characterisation of the top quark electro-weak vertices at the ILC, Eur. Phys. J. C, Volume 75 (2015), 512

[79] P. Janot Top-quark electroweak couplings at the FCC-ee, JHEP, Volume 04 (2015), 182