… }}\)) reconstruction with the ATLAS detector is evaluated using data collected in proton–proton
collisions at the LHC at a centre-of-mass energy of 13 TeV in 2015. To reconstruct\(E_ {\…

… for any hard process is that of proton–nucleon (pN) collisions (with \(\hbox {N}=\hbox {p,n}\) …
at equivalent cm energies of \(\sqrt{s_{_{\textsc {nn}}}}\approx \) 430 TeV, we show in Fig. 2 …

… This analysis is performed using a data sample of \(\hbox {pp}\) collisions at \(\sqrt{s}=13\,\…
Sources of background include top quark production (\(\hbox {t}\bar{{\hbox {t}}}\) and single top …

A search is presented for physics beyond the standard model, based on measurements of
dijet angular distributions in proton–proton collisions at\(\sqrt {s}= 13\hbox {TeV}\). The data …

… is presented based on proton–proton collision data recorded in 2011 at a centre-of-mass
energy of 7 TeV with the ATLAS detector at the LHC, and corresponding to\(4.6~\hbox {fb}^{-1}\…

… s}={13}\hbox {TeV}\) proton–proton collision data collected by the ATLAS experiment during
… are extracted, reaching as high as 2.4 TeV in gluino mass, 1.35 TeV in top-squark mass, and …

… \(\hbox {p}+{\hbox {H}_2}\) collisions for collision energies from … in \(\hbox {p}+{\hbox {H}_2}\)
collisions over a wide energy … Single ionisation cross sections for proton collisions with …

… 3.1 we present results for the proton-nucleus and nucleus-nucleus collisions for the … in the
p–\(\hbox {Bi}^{83+}\) collision at the NICA collider with the proton energy 10 GeV and the ion …

We investigate extremely rare top quark decays at a future proton–proton collider with centre-of-mass
energy of 100 TeV. We focus on two decay modes: radiative decay with a Z boson, …

… proton–proton collisions in the impact parameter b with \(0\le P(b,s) \le 1\). When the real
part of the scattering amplitude is neglected, P(b, s) is frequently denoted as \(G_\mathrm{inel}(s…