scholarly journals Framing energetic top-quark pair production at the LHC

2021 ◽  
Vol 2021 (7) ◽  
Author(s):  
Fabrizio Caola ◽  
Frédéric A. Dreyer ◽  
Ross W. McDonald ◽  
Gavin P. Salam

Abstract Top-quark pair production is central to many facets of LHC physics. At leading order, the top and anti-top are produced in a back-to-back topology, however this topology accounts only for a minority of the events with TeV-scale momentum transfer that contain a $$ t\overline{t} $$ t t ¯ pair. The remaining events instead involve the splitting of an initial or final-state gluon to $$ t\overline{t} $$ t t ¯ . We provide simple quantitative arguments that explain why this is the case, and examine the interplay between different topologies and a range of variables that characterise the event hardness. We then develop a method to classify the topologies of individual events and use it to illustrate our findings in the context of simulated events, using both top partons and suitably defined fiducial tops. For events with large $$ t\overline{t} $$ t t ¯ invariant mass, we comment on additional features that have important experimental and theoretical implications.

2021 ◽  
Vol 2021 (6) ◽  
Author(s):  
◽  
G. Aad ◽  
B. Abbott ◽  
D. C. Abbott ◽  
A. Abed Abud ◽  
...  

Abstract A search for pair production of third-generation scalar leptoquarks decaying into a top quark and a τ-lepton is presented. The search is based on a dataset of pp collisions at $$ \sqrt{s} $$ s = 13 TeV recorded with the ATLAS detector during Run 2 of the Large Hadron Collider, corresponding to an integrated luminosity of 139 fb−1. Events are selected if they have one light lepton (electron or muon) and at least one hadronically decaying τ -lepton, or at least two light leptons. In addition, two or more jets, at least one of which must be identified as containing b-hadrons, are required. Six final states, defined by the multiplicity and flavour of lepton candidates, are considered in the analysis. Each of them is split into multiple event categories to simultaneously search for the signal and constrain several leading backgrounds. The signal-rich event categories require at least one hadronically decaying τ-lepton candidate and exploit the presence of energetic final-state objects, which is characteristic of signal events. No significant excess above the Standard Model expectation is observed in any of the considered event categories, and 95% CL upper limits are set on the production cross section as a function of the leptoquark mass, for different assumptions about the branching fractions into tτ and bν. Scalar leptoquarks decaying exclusively into tτ are excluded up to masses of 1.43 TeV while, for a branching fraction of 50% into tτ, the lower mass limit is 1.22 TeV.


2015 ◽  
Vol 748 ◽  
pp. 74-78 ◽  
Author(s):  
Stefan Höche ◽  
Frank Krauss ◽  
Philipp Maierhöfer ◽  
Stefano Pozzorini ◽  
Marek Schönherr ◽  
...  

Author(s):  
S. Höche ◽  
P. Maierhöfer ◽  
N. Moretti ◽  
S. Pozzorini ◽  
F. Siegert

2003 ◽  
Vol 18 (08) ◽  
pp. 1357-1364 ◽  
Author(s):  
W. BERNREUTHER ◽  
A. BRANDENBURG ◽  
Z. G. SI ◽  
P. UWER

Top quark-antiquark [Formula: see text] pairs will be produced copiously at the Tevatron collider and in huge numbers at the LHC. This will make possible detailed investigations of the properties and interactions of this quark flavor. The analysis and interpretation of future data requires precise predictions of the hadronic production of [Formula: see text] pairs and of their subsequent decays. In this talk the reactions [Formula: see text], [Formula: see text] are considered and results are presented of our calculation6 of the dilepton angular distribution at next-to-leading order QCD, keeping the full dependence on the spins of the intermediate [Formula: see text] state. The angular distribution is determined for different choices of reference axes that can be identified with the t and [Formula: see text] spin axes. While the QCD corrections to the leading-order distribution turn out to be small in the case of the LHC, we find them to be sizeable in the case of the Tevatron and find, moreover, the angular distribution to be sensitive to the parton content of the proton.


2021 ◽  
Vol 127 (6) ◽  
Author(s):  
Javier Mazzitelli ◽  
Pier Francesco Monni ◽  
Paolo Nason ◽  
Emanuele Re ◽  
Marius Wiesemann ◽  
...  

2012 ◽  
Vol 85 (5) ◽  
Author(s):  
A. Kardos ◽  
Z. Trócsányi ◽  
C. G. Papadopoulos

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