Measurements of $t\overline{t}$ production cross-sections with the ATLAS experiment at the LHC by Margherita Spalla

“…They are performed in the dilepton, lepton+jets and the all-hadronic channels, using $\sqrt{s}=13$ TeV data from the ATLAS detector at the LHC. …”
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Parton distributions and LHC data by Rojo, J

“…Then we study the impact of the recent ATLAS and CMS W lepton asymmetry data on the NNPDF2.1 parton distributions. …”

BEYOND THE STANDARD MODEL by Ross, G

“…The implications of a heavy top quark and the origin of the light quark and lepton masses and mixing angles are considered within these frameworks.…”

WHERE DRELL-YAN BREAKS DOWN by Teper, M

“…We show that the contribution of Drell-Yan dynamics to lepton pair production at fixed x, does not scale with energy, but instead decreases as a power of the energy. …”

Light hadron spectroscopy by Close, F

“…Rapporteur talk at the Lepton-Photon Conference, Rome, July 2001: reviewing the evidence and strategies for understanding scalar mesons, glueballs and hybrids, the gluonic Pomeron and the interplay of heavy flavours and light hadron dynamics. …”

Measurement of the semileptonic decays B-bar-->D tau - nu -bar tau and B-bar-->D* tau - nu -bar tau by Fisher, Peter H., Zhao, M., Yamamoto, R. K., Taylor, Frank E., Spitznagel, M., Sciolla, Gabriella, Henderson, Shawn Wesley, Dujmic, Denis, Cowan, Ray Franklin

“…We select events with a D or D* meson and a light lepton (ℓ=e or μ) recoiling against a fully reconstructed B meson. …”
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A Solution of the Generation Puzzle from Yang-Mills Duality by Chan, H, Tsou, S

“…It predicts 3 and only 3 generations of fermions and explains the hierarchical mass spectrum as well as the main features in both the quark and lepton mixing matrices. A calculation to leading perturbative order already gives reasonable values to about half of the Standard Model parameters.…”

Performance of the DELPHI detector by Abreu, P, Adam, W, Adye, T, Agasi, E, Ajinenko, I, Aleksan, R, Alekseev, G, Alemany, R, Allport, P, Almehed, S, Alvsvaag, S, Amaldi, U, Amato, S, Andreazza, A, Andrieux, M, Antilogus, P, Apel, W, Arnoud, Y, Asman, B, Augustin, J, Augustinus, A, Baillon, P, Bambade, P, Barao, F, Barate, R

“…DELPHI (DEtector with Lepton, Photon and Hadron Identification) is a detector for e+e- physics, designed to provide high granularity over a 4π solid angle, allowing an effective particle identification. …”

Semileptonic decays $$B_{c}$$ B c meson to S-wave charmonia and X(3872) within the covariant light-front approach by Zhi-Jie Sun, Si-Yang Wang, Zhi-Qing Zhang, You-Ya Yang, Zi-Yu Zhang

“…In view of the $$R_{J/\Psi }$$ R J / Ψ anomaly released by the LHCb collaboration, it is necessary to systematically calculate the ratios $$R_X$$ R X with $$X=\psi (1S,2S,3S),\eta _c(1S,2S,3S),X(3872)$$ X = ψ ( 1 S , 2 S , 3 S ) , η c ( 1 S , 2 S , 3 S ) , X ( 3872 ) , which are helpful for checking the lepton flavor universality (LFU). We also take into account another two physical observables, the longitudinal polarization fraction $$f_{L}$$ f L and the forward–backward asymmetry $$A_{FB}$$ A FB , which can provide new clues for understanding the $$R_{J /\Psi }$$ R J / Ψ anomaly. …”
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Flavour bounds on the flavon of a minimal and a non-minimal $${\mathcal {Z}}_2 \times {\mathcal {Z}}_N$$ Z 2 × Z N symmetry by Gauhar Abbas, Vartika Singh, Neelam Singh, Ria Sain

“…The bounds on the parameter space of the flavon field of the $${\mathcal {Z}}_2 \times {\mathcal {Z}}_5$$ Z 2 × Z 5 and $${\mathcal {Z}}_2 \times {\mathcal {Z}}_9$$ Z 2 × Z 9 flavour symmetries are derived using the current quark and lepton flavour physics data and future projected sensitivities of quark and lepton flavour effects. …”
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Triple Higgs couplings in the 2HDM: the complete picture by F. Arco, S. Heinemeyer, M. J. Herrero

“…Abstract The measurement of the triple Higgs coupling is one of the main tasks of the (HL-)LHC and future lepton colliders. Similarly, triple Higgs couplings involving BSM Higgs bosons are of high interest. …”
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HIJING, a Heavy Ion Jet INteraction Generator for the High-Luminosity Era of the LHC and Beyond by Gábor Bíró, Gábor Papp, Gergely Gábor Barnaföldi, Dániel Nagy, Miklos  Gyulassy, Péter Lévai, Xin-Nian Wang, Ben-Wei Zhang

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Symmetries and Their Breaking in the Fundamental Laws of Physics by Jose Bernabeu

“…The experimental discovery of quarks and leptons and the mediators of their interactions, with physical observables in spectacular agreement with this Standard Theory, is the triumph of Symmetries. …”
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Prospects for a measurement of the W boson mass in the all-jets final state at hadron colliders by Freytsis, Marat, Hinzmann, Andreas, Moult, Ian, Tran, Nhan, Vernieri, Caterina, Harris, Philip Coleman

“…The current best measurements of the W boson mass come from single production measurements at hadron colliders in its decay mode to a lepton (electron or muon) and a neutrino and pair production of W bosons at lepton colliders, where both the leptonic and hadronic decay modes of the W boson have been considered. …”
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Search for a light pseudoscalar Higgs boson in the boosted μμττ final state in proton-proton collisions at s$$ \sqrt{s} $$ = 13 TeV by Sirunyan, A. M, Tumasyan, A., Adam, W., Ambrogi, F., Bergauer, T., Dragicevic, M., Erö, J., Escalante Del Valle, A., Frühwirth, R., Jeitler, M., Krammer, N., Lechner, L., Liko, D., Madlener, T., Mikulec, I., Rad, N., Schieck, J.

“…The ττ reconstruction efficiency is increased by modifying the standard technique for hadronic τ lepton decay reconstruction to account for a nearby muon. …”
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Search for a light pseudoscalar Higgs boson in the boosted μμττ final state in proton-proton collisions at s$$ \sqrt{s} $$ = 13 TeV by Sirunyan, A. M, Tumasyan, A., Adam, W., Ambrogi, F., Bergauer, T., Dragicevic, M., Erö, J., Escalante Del Valle, A., Frühwirth, R., Jeitler, M., Krammer, N., Lechner, L., Liko, D., Madlener, T., Mikulec, I., Rad, N., Schieck, J.

“…The ττ reconstruction efficiency is increased by modifying the standard technique for hadronic τ lepton decay reconstruction to account for a nearby muon. …”
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Measurement of the top quark mass using events with a single reconstructed top quark in pp collisions at... by Tumasyan, A., Adam, W., Andrejkovic, J. W., Bergauer, T., Chatterjee, S., Dragicevic, M., Escalante Del Valle, A., Frühwirth, R., Jeitler, M., Krammer, N., Lechner, L., Liko, D., Mikulec, I., Paulitsch, P., Pitters, F. M., Schieck, J., Schöfbeck, R., Spanring, M.

“…Candidate events are selected by requiring an isolated high-momentum lepton (muon or electron) and exactly two jets, of which one is identified as originating from a bottom quark. …”
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Precision Measurements of the Vector Boson Scattering Production and Searches for Charged Higgs Bosons at the Large Hadron Collider by Hu, Miao

“…In the leptonic channel, differential fiducial cross sections as functions of the invariant masses of the jet and charged lepton pairs, as well as of the leading-lepton transverse momentum, are measured for [formula] production, and as a function of the invariant mass of the jet pair is also measured for WZ production. …”
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Search for supersymmetry in final states with a single electron or muon using angular correlations and heavy-object identification in proton-proton collisions at √𝑠 = 13 TeV by Tumasyan, A., Adam, W., Andrejkovic, J. W., Bergauer, T., Chatterjee, S., Damanakis, K., Dragicevic, M., Escalante Del Valle, A., Hussain, P. S., Jeitler, M., Krammer, N., Lechner, L., Liko, D., Mikulec, I., Paulitsch, P., Pitters, F. M., Schieck, J., Schöfbeck, R.

“…Abstract A search for supersymmetry is presented in events with a single charged lepton, electron or muon, and multiple hadronic jets. …”
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Search for supersymmetry in final states with a single electron or muon using angular correlations and heavy-object identification in proton-proton collisions at... by Tumasyan, A., Adam, W., Andrejkovic, J. W., Bergauer, T., Chatterjee, S., Damanakis, K., Dragicevic, M., Escalante Del Valle, A., Hussain, P. S., Jeitler, M., Krammer, N., Lechner, L., Liko, D., Mikulec, I., Paulitsch, P., Pitters, F. M., Schieck, J., Schöfbeck, R.

“…A search for supersymmetry is presented in events with a single charged lepton, electron or muon, and multiple hadronic jets. …”
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