Erratum to: Search for single top-quark production via flavour-changing neutral currents at 8 TeV with the ATLAS detector

The European Physical Journal C

Published On 2022/1

One correction is noted for the paper. The branching fraction was not included in the conversion of the observed cross-section limit, pb to the coupling constants and and the branching fractions and. The inclusion leads to weaker observed exclusion limits on the coupling constants divided by the scale of new physics of and and on the branching fractions and. The predicted exclusion limits on the coupling constants divided by the scale of new physics are and and on the branching fractions and. Updated distributions of the observed upper limits on the coupling constants for combinations of cgt and ugt channels are shown in Figure 10 a and on the branching fractions in Figure 10 b.

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The European Physical Journal C

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2022/1

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82

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1

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1-15

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Silvia Behar Harpaz

Silvia Behar Harpaz

Technion - Israel Institute of Technology

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High Energy Physics

Robert W. Gardner Jr

Robert W. Gardner Jr

University of Chicago

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Physical Sciences Division

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250

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159

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High Energy Physics

Distributed Computing

Advanced Cyberinfrastructure

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Michael Kobel

Michael Kobel

Technische Universität Dresden

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Professor der Physik

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243

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Elementarteilchenphysik

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Karlheinz Meier

Karlheinz Meier

Heidelberg University

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146

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Physics instrumentation

particle physics

physical foundations of information processing

brain-inspired computing

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Martín Fernando Tripiana

Martín Fernando Tripiana

Universidad Nacional de La Plata

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Doctor en Física Facultad de Ciencias Exactas

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David Wardrope

David Wardrope

University College London

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Harry Williams

Harry Williams

University of North Texas

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Simon Viel

Simon Viel

Carleton University

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Assistant Professor of Physics

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Arindam Lala

Arindam Lala

Pontificia Universidad Católica de Valparaíso

The European Physical Journal C

Non-chaotic dynamics for Yang–Baxter deformed superstrings

We explore a novel class of Yang–Baxter deformed backgrounds (J High Energy Phys 01:056, 2021) which exhibit a non-chaotic dynamics for (super)strings propagating over it. We explicitly use the Kovacic’s algorithm in order to establish non-chaotic dynamics of string models over these deformed backgrounds. This analysis is complemented with numerical techniques whereby we probe the classical phase space of these (semi)classical strings and calculate various chaos indicators, such as, the Poincaré sections and the Lyapunov exponents. We find compatibility between the two approaches. Nevertheless, our analysis does not ensure integrability; rather, it excludes the possibility of non-integrability for the given string embeddings.

Giuseppe Callea

Giuseppe Callea

University of Glasgow

The European Physical Journal C

Measurement of the and cross-sections in pp collisions at TeV with the ATLAS detector

The inclusive Higgs boson production cross-section is measured in the di-photon and the decay channels using 31.4 and 29.0 fb of pp collision data respectively, collected with the ATLAS detector at a centre-of-mass energy of  . To reduce the model dependence, the measurement in each channel is restricted to a particle-level phase space that closely matches the channel’s detector-level kinematic selection, and it is corrected for detector effects. These measured fiducial cross-sections are   fb, and   fb, in agreement with the corresponding Standard Model predictions of  fb and  fb. Assuming Standard Model acceptances and branching fractions for the two channels, the fiducial measurements are extrapolated to the full phase space yielding total cross-sections of  pb and  pb at 13.6  from the di-photon and  …

Giuseppe Callea

Giuseppe Callea

University of Glasgow

The European Physical Journal C

Measurement of the production cross-section of and mesons in pp collisions at  TeV with the ATLAS detector

Measurements of the differential production cross-sections of prompt and non-prompt and mesons with transverse momenta between 8 and 360 GeV and rapidity in the range are reported. Furthermore, measurements of the non-prompt fractions of and , and the prompt and non-prompt -to- production ratios, are presented. The analysis is performed using 140 fb of  TeV pp collision data recorded by the ATLAS detector at the LHC during the years 2015–2018.

Giuseppe Callea

Giuseppe Callea

University of Glasgow

The European Physical Journal C

Search for invisible particles produced in association with single top quarks in proton-proton collisions at =13 TeV with the ATLAS detector

A search for the production of single-top-quarks in association with missing energy is performed in proton–proton collisions at a centre-of-mass energy of with the ATLAS experiment at the large hadron collider using data collected in 2012, corresponding to an integrated luminosity of  fb. In this search, the boson from the top quark is required to decay into an electron or a muon and a neutrino. No deviation from the standard model prediction is observed, and upper limits are set on the production cross-section for resonant and non-resonant production of an invisible exotic state in association with a right-handed top quark. In the case of resonant production, for a spin- resonance with a mass of  GeV, an effective coupling strength above is excluded at 95 confidence level for the top quark and an invisible spin- state with mass between and  GeV. In the case of non-resonant production, an effective …

Giuseppe Callea

Giuseppe Callea

University of Glasgow

The European Physical Journal C

A precise measurement of the Z-boson double-differential transverse momentum and rapidity distributions in the full phase space of the decay leptons with the ATLAS …

This paper presents for the first time a precise measurement of the production properties of the Z boson in the full phase space of the decay leptons. This is in contrast to the many previous precise unfolded measurements performed in the fiducial phase space of the decay leptons. The measurement is obtained from proton–proton collision data collected by the ATLAS experiment in 2012 at TeV at the LHC and corresponding to an integrated luminosity of 20.2 fb. The results, based on a total of 15.3 million Z-boson decays to electron and muon pairs, extend and improve a previous measurement of the full set of angular coefficients describing Z-boson decay. The double-differential cross-section distributions in Z-boson transverse momentum  and rapidity  are measured in the pole region, defined as GeV, over the range . The total uncertainty of the normalised cross-section measurements in the peak region of the …

Amitkumar Mehta

Amitkumar Mehta

University of Alabama at Birmingham

The European Physical Journal C

Impact of beam–beam effects on absolute luminosity calibrations at the CERN Large Hadron Collider

At the Large Hadron Collider (LHC), absolute luminosity calibrations obtained by the van der Meer (vdM) method are affected by the mutual electromagnetic interaction of the two beams. The colliding bunches experience relative orbit shifts, as well as optical distortions akin to the dynamic- effect, that both depend on the transverse beam separation and must therefore be corrected for when deriving the absolute luminosity scale. In the vdM regime, the beam–beam parameter is small enough that the orbit shift can be calculated analytically. The dynamic- corrections to the luminometer calibrations, however, had until the end of Run 2 been estimated in the linear approximation only. In this report, the influence of beam–beam effects on the vdM-based luminosity scale is quantified, together with the associated systematic uncertainties, by means of simulations that fully take into account the non-linearity of the beam …

Ignacio J. Araya

Ignacio J. Araya

Universidad Arturo Prat

The European Physical Journal C

Weyl–invariant scalar–tensor gravities from purely metric theories

We describe a method to generate scalar–tensor theories with Weyl symmetry, starting from arbitrary purely metric higher derivative gravity theories. The method consists in the definition of a conformally-invariant metric, that is a rank (0, 2)-tensor constructed out of the metric tensor and the scalar field. This new object has zero conformal weight and is given by, where is the conformal dimension of the scalar. As has conformal dimension of 2, the resulting tensor is trivially a conformal invariant. Then, the generated scalar–tensor theory, which we call the Weyl uplift of the original purely metric theory, is obtained by replacing the metric by in the action that defines the original theory. This prescription allowed us to define the Weyl uplift of theories with terms of higher order in the Riemannian curvature. Furthermore, the prescription for scalar–tensor theories coming from terms that have explicit …

Giorgos Anastasiou

Giorgos Anastasiou

Pontificia Universidad Católica de Valparaíso

The European Physical Journal C

Weyl–invariant scalar–tensor gravities from purely metric theories

We describe a method to generate scalar–tensor theories with Weyl symmetry, starting from arbitrary purely metric higher derivative gravity theories. The method consists in the definition of a conformally-invariant metric, that is a rank (0, 2)-tensor constructed out of the metric tensor and the scalar field. This new object has zero conformal weight and is given by, where is the conformal dimension of the scalar. As has conformal dimension of 2, the resulting tensor is trivially a conformal invariant. Then, the generated scalar–tensor theory, which we call the Weyl uplift of the original purely metric theory, is obtained by replacing the metric by in the action that defines the original theory. This prescription allowed us to define the Weyl uplift of theories with terms of higher order in the Riemannian curvature. Furthermore, the prescription for scalar–tensor theories coming from terms that have explicit …

David W. Miller

David W. Miller

University of Chicago

The European Physical Journal C

Measurement of the and cross-sections in pp collisions at TeV with the ATLAS detector

The inclusive Higgs boson production cross-section is measured in the di-photon and the decay channels using 31.4 and 29.0 fb of pp collision data respectively, collected with the ATLAS detector at a centre-of-mass energy of  . To reduce the model dependence, the measurement in each channel is restricted to a particle-level phase space that closely matches the channel’s detector-level kinematic selection, and it is corrected for detector effects. These measured fiducial cross-sections are   fb, and   fb, in agreement with the corresponding Standard Model predictions of  fb and  fb. Assuming Standard Model acceptances and branching fractions for the two channels, the fiducial measurements are extrapolated to the full phase space yielding total cross-sections of  pb and  pb at 13.6  from the di-photon and  …

David W. Miller

David W. Miller

University of Chicago

The European Physical Journal C

Measurement of the production cross-section of and mesons in pp collisions at  TeV with the ATLAS detector

Measurements of the differential production cross-sections of prompt and non-prompt and mesons with transverse momenta between 8 and 360 GeV and rapidity in the range are reported. Furthermore, measurements of the non-prompt fractions of and , and the prompt and non-prompt -to- production ratios, are presented. The analysis is performed using 140 fb of  TeV pp collision data recorded by the ATLAS detector at the LHC during the years 2015–2018.