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  • Energy Research

  • Measurement of isolated-photon plus two-jet production in pp collisions at $$ \sqrt{s} $$ = 13 TeV with the ATLAS detector

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    descriptionPublicationkeyboard_double_arrow_right Article , Preprint , Other literature type , Journal 2020Embargo end date: 01 Jan 2019 France, Netherlands, South Africa, United Kingdom, Italy, Poland, Italy, United Kingdom, Italy, Netherlands, Turkey, Italy, Spain, Portugal, Italy, Belarus, Netherlands, Norway, United Kingdom, Italy, Sweden, Germany, Italy, Spain, Germany, Turkey, Italy, Belarus, Netherlands, Czech Republic, China (People's Republic of), Italy, Italy, Italy, Italy, Chile, Czech Republic, Germany, Netherlands, China (People's Republic of), Spain, South Africa, Turkey, Norway, Germany, United Kingdom, China (People's Republic of), Italy, Australia, Denmark, Turkey, Australia, Australia, Italy, Italy, United States, Turkey Publisher:Springer Science and Business Media LLCFunded by:EC | PROBIST, GSRI
    Authors: Aad, Georges; Abbott, Brad; Abreu, Henso; Araujo Ferraz, Victor; +196 Authors

    doi: 10.1007/jhep03(2020)179 , 10.3204/pubdb-2020-02525 , 10.48550/arxiv.1912.09866 , 10.17863/cam.66468 , 10.17863/cam.53552 , 10.17863/cam.69498

    arXiv: 1912.09866 , http://arxiv.org/abs/1912.09866

    handle: 2066/218361 , https://repository.ubn.ru.nl/handle/2066/218361 , 11588/884357 , 11245.1/18bc9ce6-7e36-4673-bd77-df314f6020ed , 20.500.11851/9303 , 10852/83588 , 11250/2756168 , 10261/232887 , 10316/106311 , 10486/708879 , 10481/61851 , 20.500.11770/304198 , 11572/317931 , 11390/1182228 , 2108/275731 , 11590/388554 , 11573/1493191 , 11367/95123 , 11567/1103136 , 11568/1076219 , 11587/427313 , 11585/790275 , 1959.3/463676 , 11571/1370394 , 11343/252034 , 10210/463537 , 11411/2003

    Abstract The dynamics of isolated-photon plus two-jet production in pp collisions at a centre-of-mass energy of 13 TeV are studied with the ATLAS detector at the LHC using a dataset corresponding to an integrated luminosity of 36.1 fb−1. Cross sections are measured as functions of a variety of observables, including angular correlations and invariant masses of the objects in the final state, γ + jet + jet. Measurements are also performed in phase-space regions enriched in each of the two underlying physical mechanisms, namely direct and fragmentation processes. The measurements cover the range of photon (jet) transverse momenta from 150 GeV (100 GeV) to 2 TeV. The tree-level plus parton-shower predictions from Sherpa and Pythia as well as the next-to-leading-order QCD predictions from Sherpa are compared with the measurements. The next-to-leading-order QCD predictions describe the data adequately in shape and normalisation except for regions of phase space such as those with high values of the invariant mass or rapidity separation of the two jets, where the predictions overestimate the data.

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    CORE
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    CORE (RIOXX-UK Aggregator)
    Article . 2020
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    Archivio istituzionale della ricerca - Università degli Studi di Udine
    Article . 2020
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      Claim

      This Research product is the result of merged Research products in OpenAIRE.

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  • Measurement of isolated-photon plus two-jet production in pp collisions at $$ \sqrt{s} $$ = 13 TeV with the ATLAS detector

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    descriptionPublicationkeyboard_double_arrow_right Article , Preprint , Other literature type , Journal 2020Embargo end date: 01 Jan 2019 France, Netherlands, South Africa, United Kingdom, Italy, Poland, Italy, United Kingdom, Italy, Netherlands, Turkey, Italy, Spain, Portugal, Italy, Belarus, Netherlands, Norway, United Kingdom, Italy, Sweden, Germany, Italy, Spain, Germany, Turkey, Italy, Belarus, Netherlands, Czech Republic, China (People's Republic of), Italy, Italy, Italy, Italy, Chile, Czech Republic, Germany, Netherlands, China (People's Republic of), Spain, South Africa, Turkey, Norway, Germany, United Kingdom, China (People's Republic of), Italy, Australia, Denmark, Turkey, Australia, Australia, Italy, Italy, United States, Turkey Publisher:Springer Science and Business Media LLCFunded by:EC | PROBIST, GSRI
    Authors: Aad, Georges; Abbott, Brad; Abreu, Henso; Araujo Ferraz, Victor; +196 Authors

    doi: 10.1007/jhep03(2020)179 , 10.3204/pubdb-2020-02525 , 10.48550/arxiv.1912.09866 , 10.17863/cam.66468 , 10.17863/cam.53552 , 10.17863/cam.69498

    arXiv: 1912.09866 , http://arxiv.org/abs/1912.09866

    handle: 2066/218361 , https://repository.ubn.ru.nl/handle/2066/218361 , 11588/884357 , 11245.1/18bc9ce6-7e36-4673-bd77-df314f6020ed , 20.500.11851/9303 , 10852/83588 , 11250/2756168 , 10261/232887 , 10316/106311 , 10486/708879 , 10481/61851 , 20.500.11770/304198 , 11572/317931 , 11390/1182228 , 2108/275731 , 11590/388554 , 11573/1493191 , 11367/95123 , 11567/1103136 , 11568/1076219 , 11587/427313 , 11585/790275 , 1959.3/463676 , 11571/1370394 , 11343/252034 , 10210/463537 , 11411/2003

    Abstract The dynamics of isolated-photon plus two-jet production in pp collisions at a centre-of-mass energy of 13 TeV are studied with the ATLAS detector at the LHC using a dataset corresponding to an integrated luminosity of 36.1 fb−1. Cross sections are measured as functions of a variety of observables, including angular correlations and invariant masses of the objects in the final state, γ + jet + jet. Measurements are also performed in phase-space regions enriched in each of the two underlying physical mechanisms, namely direct and fragmentation processes. The measurements cover the range of photon (jet) transverse momenta from 150 GeV (100 GeV) to 2 TeV. The tree-level plus parton-shower predictions from Sherpa and Pythia as well as the next-to-leading-order QCD predictions from Sherpa are compared with the measurements. The next-to-leading-order QCD predictions describe the data adequately in shape and normalisation except for regions of phase space such as those with high values of the invariant mass or rapidity separation of the two jets, where the predictions overestimate the data.

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    CORE
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    CORE (RIOXX-UK Aggregator)
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    Archivio istituzionale della ricerca - Università degli Studi di Udine
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  • Measurement of the $$t\bar{t}$$ production cross-section and lepton differential distributions in $$e\mu $$ dilepton events from pp collisions at $$\sqrt{s}=13\,\text {TeV}$$ with the ATLAS detector

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    descriptionPublicationkeyboard_double_arrow_right Article , Research , Preprint , Other literature type , Journal 2020Embargo end date: 01 Jan 2019 France, Switzerland, Turkey, China (People's Republic of), Italy, Australia, Netherlands, Italy, Norway, Netherlands, Italy, Italy, Turkey, Australia, Spain, United States, Norway, United Kingdom, Italy, Netherlands, Italy, Denmark, Italy, Italy, Sweden, Germany, United Kingdom, Netherlands, Italy, Spain, Germany, Portugal, China (People's Republic of), Australia, Italy, Italy, Netherlands, Czech Republic, Turkey, Spain, Chile, Italy, China (People's Republic of), Turkey, Czech Republic, Poland, United Kingdom, Italy, Italy, United Kingdom, Italy, Germany Publisher:Springer Science and Business Media LLCFunded by:EC | PROBIST
    Authors: Aad, Georges; Abbott, Brad; Abreu, Henso; Arcangeletti, Chiara; +196 Authors

    doi: 10.1140/epjc/s10052-020-7907-9 , 10.48550/arxiv.1910.08819 , 10.3204/pubdb-2019-05253 , 10.17863/cam.54305 , 10.17863/cam.56336 , 10.17863/cam.53878 , 10.17863/cam.71238 , 10.3204/pubdb-2020-02552 , 10.17863/cam.55182

    arXiv: 1910.08819 , http://arxiv.org/abs/1910.08819

    handle: 2066/221204 , 2066/221923 , https://repository.ubn.ru.nl/handle/2066/221204 , 11588/884416 , 11245.1/63948321-7440-4575-bbe9-d7fcb633bb42 , 20.500.11851/9777 , 11250/2755506 , 10852/83795 , 10261/232448 , 10316/106040 , 10486/704298 , 10481/64525 , 20.500.11770/306706 , 11572/318659 , 11390/1187851 , 2108/275805 , 11590/388717 , 11573/1494293 , 11367/95174 , 11567/1034593 , 11568/1075979 , 11587/439702 , 11585/783052 , 11343/252094 , 11571/1370850 , 1959.3/463769

    AbstractThe inclusive top quark pair ($$t\bar{t}$$ t t ¯ ) production cross-section $$\sigma _{t\bar{t}}$$ σ t t ¯ has been measured in proton–proton collisions at $$\sqrt{s}=13\,\text {TeV}$$ s = 13 TeV , using 36.1 fb$$^{-1}$$ - 1 of data collected in 2015–2016 by the ATLAS experiment at the LHC. Using events with an opposite-charge $$e\mu $$ e μ pair and b-tagged jets, the cross-section is measured to be: $$\begin{aligned} \sigma _{t\bar{t}} = 826.4 \pm 3.6\,\mathrm {(stat)}\ \pm 11.5\,\mathrm {(syst)}\ \pm 15.7\,\mathrm {(lumi)}\ \pm 1.9\,\mathrm {(beam)}\,\mathrm {pb}, \end{aligned}$$ σ t t ¯ = 826.4 ± 3.6 ( stat ) ± 11.5 ( syst ) ± 15.7 ( lumi ) ± 1.9 ( beam ) pb , where the uncertainties reflect the limited size of the data sample, experimental and theoretical systematic effects, the integrated luminosity, and the LHC beam energy, giving a total uncertainty of 2.4%. The result is consistent with theoretical QCD calculations at next-to-next-to-leading order. It is used to determine the top quark pole mass via the dependence of the predicted cross-section on $$m_t^{\mathrm{pole}}$$ m t pole , giving $$m_t^{\mathrm{pole}}=173.1^{+2.0}_{-2.1}\,\text {GeV}$$ m t pole = 173 . 1 - 2.1 + 2.0 GeV . It is also combined with measurements at $$\sqrt{s}=7\,\text {TeV}$$ s = 7 TeV and $$\sqrt{s}=8\,\text {TeV}$$ s = 8 TeV to derive ratios and double ratios of $$t\bar{t}$$ t t ¯ and Z cross-sections at different energies. The same event sample is used to measure absolute and normalised differential cross-sections as functions of single-lepton and dilepton kinematic variables, and the results are compared with predictions from various Monte Carlo event generators.

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      Claim

      This Research product is the result of merged Research products in OpenAIRE.

      You have already added works in your ORCID record related to the merged Research product.

  • Measurement of the $$t\bar{t}$$ production cross-section and lepton differential distributions in $$e\mu $$ dilepton events from pp collisions at $$\sqrt{s}=13\,\text {TeV}$$ with the ATLAS detector

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    descriptionPublicationkeyboard_double_arrow_right Article , Research , Preprint , Other literature type , Journal 2020Embargo end date: 01 Jan 2019 France, Switzerland, Turkey, China (People's Republic of), Italy, Australia, Netherlands, Italy, Norway, Netherlands, Italy, Italy, Turkey, Australia, Spain, United States, Norway, United Kingdom, Italy, Netherlands, Italy, Denmark, Italy, Italy, Sweden, Germany, United Kingdom, Netherlands, Italy, Spain, Germany, Portugal, China (People's Republic of), Australia, Italy, Italy, Netherlands, Czech Republic, Turkey, Spain, Chile, Italy, China (People's Republic of), Turkey, Czech Republic, Poland, United Kingdom, Italy, Italy, United Kingdom, Italy, Germany Publisher:Springer Science and Business Media LLCFunded by:EC | PROBIST
    Authors: Aad, Georges; Abbott, Brad; Abreu, Henso; Arcangeletti, Chiara; +196 Authors

    doi: 10.1140/epjc/s10052-020-7907-9 , 10.48550/arxiv.1910.08819 , 10.3204/pubdb-2019-05253 , 10.17863/cam.54305 , 10.17863/cam.56336 , 10.17863/cam.53878 , 10.17863/cam.71238 , 10.3204/pubdb-2020-02552 , 10.17863/cam.55182

    arXiv: 1910.08819 , http://arxiv.org/abs/1910.08819

    handle: 2066/221204 , 2066/221923 , https://repository.ubn.ru.nl/handle/2066/221204 , 11588/884416 , 11245.1/63948321-7440-4575-bbe9-d7fcb633bb42 , 20.500.11851/9777 , 11250/2755506 , 10852/83795 , 10261/232448 , 10316/106040 , 10486/704298 , 10481/64525 , 20.500.11770/306706 , 11572/318659 , 11390/1187851 , 2108/275805 , 11590/388717 , 11573/1494293 , 11367/95174 , 11567/1034593 , 11568/1075979 , 11587/439702 , 11585/783052 , 11343/252094 , 11571/1370850 , 1959.3/463769

    AbstractThe inclusive top quark pair ($$t\bar{t}$$ t t ¯ ) production cross-section $$\sigma _{t\bar{t}}$$ σ t t ¯ has been measured in proton–proton collisions at $$\sqrt{s}=13\,\text {TeV}$$ s = 13 TeV , using 36.1 fb$$^{-1}$$ - 1 of data collected in 2015–2016 by the ATLAS experiment at the LHC. Using events with an opposite-charge $$e\mu $$ e μ pair and b-tagged jets, the cross-section is measured to be: $$\begin{aligned} \sigma _{t\bar{t}} = 826.4 \pm 3.6\,\mathrm {(stat)}\ \pm 11.5\,\mathrm {(syst)}\ \pm 15.7\,\mathrm {(lumi)}\ \pm 1.9\,\mathrm {(beam)}\,\mathrm {pb}, \end{aligned}$$ σ t t ¯ = 826.4 ± 3.6 ( stat ) ± 11.5 ( syst ) ± 15.7 ( lumi ) ± 1.9 ( beam ) pb , where the uncertainties reflect the limited size of the data sample, experimental and theoretical systematic effects, the integrated luminosity, and the LHC beam energy, giving a total uncertainty of 2.4%. The result is consistent with theoretical QCD calculations at next-to-next-to-leading order. It is used to determine the top quark pole mass via the dependence of the predicted cross-section on $$m_t^{\mathrm{pole}}$$ m t pole , giving $$m_t^{\mathrm{pole}}=173.1^{+2.0}_{-2.1}\,\text {GeV}$$ m t pole = 173 . 1 - 2.1 + 2.0 GeV . It is also combined with measurements at $$\sqrt{s}=7\,\text {TeV}$$ s = 7 TeV and $$\sqrt{s}=8\,\text {TeV}$$ s = 8 TeV to derive ratios and double ratios of $$t\bar{t}$$ t t ¯ and Z cross-sections at different energies. The same event sample is used to measure absolute and normalised differential cross-sections as functions of single-lepton and dilepton kinematic variables, and the results are compared with predictions from various Monte Carlo event generators.

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  • Measurement of the cross section for isolated-photon plus jet production in $pp$ collisions at $\sqrt s=13$ TeV using the ATLAS detector

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    descriptionPublicationkeyboard_double_arrow_right Article , Research , Preprint , Journal , Other literature type 2017Embargo end date: 01 Jan 2018 Italy, Italy, Turkey, Germany, France, United Kingdom, Italy, United Kingdom, Germany, Germany, South Africa, South Africa, Italy, Turkey, United Kingdom, United Kingdom, United Kingdom, Italy, Switzerland, Italy, United Kingdom, United Kingdom, Italy, Italy, Italy, Italy Publisher:arXivFunded by:GSRI
    Authors: Jeannine Wagner-kuhr; Juraj Bracinik; Yoichi Ninomiya; Pavel Starovoitov; +196 Authors

    doi: 10.48550/arxiv.1801.00112 , 10.3204/pubdb-2018-00059 , 10.3204/pubdb-2018-01922

    arXiv: http://arxiv.org/abs/1801.00112 , 1801.00112

    handle: 2434/587256 , 20.500.11770/304349 , 11390/1131440 , 2108/200863 , 11590/337685 , 11573/1216320 , 11367/72188 , 11568/947245 , 11568/1164402 , 11571/1271006 , 10210/287612

    The dynamics of isolated-photon production in association with a jet in proton–proton collisions at a centre-of-mass energy of 13 TeV are studied with the ATLAS detector at the LHC using a dataset with an integrated luminosity of 3.2 $fb^{−1}$. Photons are required to have transverse energies above 125 GeV. Jets are identified using the anti-$k_t$ algorithm with radius parameter $R = 0.4$ and required to have transverse momenta above 100 GeV. Measurements of isolated-photon plus jet cross sections are presented as functions of the leading-photon transverse energy, the leading-jet transverse momentum, the azimuthal angular separation between the photon and the jet, the photon–jet invariant mass and the scattering angle in the photon–jet centre-of-mass system. Tree-level plus parton-shower predictions from Sherpa and Pythia as well as next-to-leading-order QCD predictions from Jetphox and Sherpa are compared to the measurements. Physics letters / B 780, 578 - 602 (2018). doi:10.1016/j.physletb.2018.03.035 Published by North-Holland Publ., Amsterdam

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  • Measurement of the cross section for isolated-photon plus jet production in $pp$ collisions at $\sqrt s=13$ TeV using the ATLAS detector

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    descriptionPublicationkeyboard_double_arrow_right Article , Research , Preprint , Journal , Other literature type 2017Embargo end date: 01 Jan 2018 Italy, Italy, Turkey, Germany, France, United Kingdom, Italy, United Kingdom, Germany, Germany, South Africa, South Africa, Italy, Turkey, United Kingdom, United Kingdom, United Kingdom, Italy, Switzerland, Italy, United Kingdom, United Kingdom, Italy, Italy, Italy, Italy Publisher:arXivFunded by:GSRI
    Authors: Jeannine Wagner-kuhr; Juraj Bracinik; Yoichi Ninomiya; Pavel Starovoitov; +196 Authors

    doi: 10.48550/arxiv.1801.00112 , 10.3204/pubdb-2018-00059 , 10.3204/pubdb-2018-01922

    arXiv: http://arxiv.org/abs/1801.00112 , 1801.00112

    handle: 2434/587256 , 20.500.11770/304349 , 11390/1131440 , 2108/200863 , 11590/337685 , 11573/1216320 , 11367/72188 , 11568/947245 , 11568/1164402 , 11571/1271006 , 10210/287612

    The dynamics of isolated-photon production in association with a jet in proton–proton collisions at a centre-of-mass energy of 13 TeV are studied with the ATLAS detector at the LHC using a dataset with an integrated luminosity of 3.2 $fb^{−1}$. Photons are required to have transverse energies above 125 GeV. Jets are identified using the anti-$k_t$ algorithm with radius parameter $R = 0.4$ and required to have transverse momenta above 100 GeV. Measurements of isolated-photon plus jet cross sections are presented as functions of the leading-photon transverse energy, the leading-jet transverse momentum, the azimuthal angular separation between the photon and the jet, the photon–jet invariant mass and the scattering angle in the photon–jet centre-of-mass system. Tree-level plus parton-shower predictions from Sherpa and Pythia as well as next-to-leading-order QCD predictions from Jetphox and Sherpa are compared to the measurements. Physics letters / B 780, 578 - 602 (2018). doi:10.1016/j.physletb.2018.03.035 Published by North-Holland Publ., Amsterdam

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    Other literature type . 2017
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    Archivio della Ricerca - Università di Roma Tor vergata
    Article . 2018
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    Article . 2018
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    Article . 2018
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    Article . 2018
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    Archivio istituzionale della ricerca - Università degli Studi di Udine
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    Archivio della Ricerca - Università degli Studi Roma Tre
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    Archivio della ricerca- Università di Roma La Sapienza
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    Archivio della ricerca - Università degli studi di Napoli "Parthenope"
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    Archivio della Ricerca - Università di Pisa
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    Archivio della Ricerca - Università di Roma Tor vergata
    Article . 2018
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    Research . 2017
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    HAL-IN2P3 (Institut national de physique nucléaire et de physique des particules)
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    Université Savoie Mont Blanc: HAL
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      Archivio Istituzionale della Ricerca dell'Università degli Studi di Milano
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      Article . 2018
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      Archivio della ricerca- Università di Roma La Sapienza
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      Archivio della ricerca - Università degli studi di Napoli "Parthenope"
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  • The energy spectrum of cosmic rays beyond the turn-down around $$\varvec{10^{17}}$$ eV as measured with the surface detector of the Pierre Auger Observatory

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    Authors: G. Medina-Tanco; J. Stasielak; G. Farrar; Trent D. Grubb; +196 Authors

    doi: 10.1140/epjc/s10052-021-09700-w , 10.48550/arxiv.2109.13400 , 10.18154/rwth-2021-12100 , 10.18154/rwth-2022-00047

    arXiv: http://arxiv.org/abs/2109.13400 , 2109.13400

    handle: https://repository.ubn.ru.nl/handle/2066/239867 , 11588/890384 , 11245.1/e277820a-6074-4fdc-9cd2-9d87842d0efe , 2066/239867 , 2434/1033134 , 10481/71942 , 20.500.12556/RUNG-6965 , 11311/1189557 , 20.500.14017/fb76dc10-e5e8-4ff6-88c2-75af44762dfb , 11697/176134 , 11587/458363 , 20.500.11769/526705 , 2318/1841975 , 2133/23683

    AbstractWe present a measurement of the cosmic-ray spectrum above 100 PeV using the part of the surface detector of the Pierre Auger Observatory that has a spacing of 750 m. An inflection of the spectrum is observed, confirming the presence of the so-called second-knee feature. The spectrum is then combined with that of the 1500 m array to produce a single measurement of the flux, linking this spectral feature with the three additional breaks at the highest energies. The combined spectrum, with an energy scale set calorimetrically via fluorescence telescopes and using a single detector type, results in the most statistically and systematically precise measurement of spectral breaks yet obtained. These measurements are critical for furthering our understanding of the highest energy cosmic rays.

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  • The energy spectrum of cosmic rays beyond the turn-down around $$\varvec{10^{17}}$$ eV as measured with the surface detector of the Pierre Auger Observatory

    image/svg+xml art designer at PLoS, modified by Wikipedia users Nina, Beao, JakobVoss, and AnonMoos Open Access logo, converted into svg, designed by PLoS. This version with transparent background. http://commons.wikimedia.org/wiki/File:Open_Access_logo_PLoS_white.svg art designer at PLoS, modified by Wikipedia users Nina, Beao, JakobVoss, and AnonMoos http://www.plos.org/
    descriptionPublicationkeyboard_double_arrow_right Article , Research , Preprint , Journal 2021Embargo end date: 01 Jan 2021 Netherlands, Italy, Slovenia, Netherlands, Spain, Czech Republic, Italy, Italy, Italy, Argentina, Netherlands, Netherlands, France, Italy, Germany, Czech Republic, Belgium, Italy, Argentina, Italy, Germany, Netherlands Publisher:Springer Science and Business Media LLCFunded by:NSF | Pierre Auger Project, ANR | SUPER
    Authors: G. Medina-Tanco; J. Stasielak; G. Farrar; Trent D. Grubb; +196 Authors

    doi: 10.1140/epjc/s10052-021-09700-w , 10.48550/arxiv.2109.13400 , 10.18154/rwth-2021-12100 , 10.18154/rwth-2022-00047

    arXiv: http://arxiv.org/abs/2109.13400 , 2109.13400

    handle: https://repository.ubn.ru.nl/handle/2066/239867 , 11588/890384 , 11245.1/e277820a-6074-4fdc-9cd2-9d87842d0efe , 2066/239867 , 2434/1033134 , 10481/71942 , 20.500.12556/RUNG-6965 , 11311/1189557 , 20.500.14017/fb76dc10-e5e8-4ff6-88c2-75af44762dfb , 11697/176134 , 11587/458363 , 20.500.11769/526705 , 2318/1841975 , 2133/23683

    AbstractWe present a measurement of the cosmic-ray spectrum above 100 PeV using the part of the surface detector of the Pierre Auger Observatory that has a spacing of 750 m. An inflection of the spectrum is observed, confirming the presence of the so-called second-knee feature. The spectrum is then combined with that of the 1500 m array to produce a single measurement of the flux, linking this spectral feature with the three additional breaks at the highest energies. The combined spectrum, with an energy scale set calorimetrically via fluorescence telescopes and using a single detector type, results in the most statistically and systematically precise measurement of spectral breaks yet obtained. These measurements are critical for furthering our understanding of the highest energy cosmic rays.

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  • Measurement of the $Z(\rightarrow\ell^+\ell^-)\gamma$ production cross-section in $pp$ collisions at $\sqrt{s} =13$ TeV with the ATLAS detector

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    descriptionPublicationkeyboard_double_arrow_right Article , Research , Preprint 2019 Germany, France, Germany Publisher:Deutsches Elektronen-Synchrotron, DESY, Hamburg
    Authors: Aad, Georges; Abbott, Brad; Abreu, Henso; Araujo Pereira, Rodrigo; +196 Authors

    doi: 10.3204/pubdb-2020-02534 , 10.3204/pubdb-2019-05270

    arXiv: http://arxiv.org/abs/1911.04813 , 1911.04813

    The production of a prompt photon in association with a $Z$ boson is studied in proton-proton collisions at a centre-of-mass energy $\sqrt{s} =$ 13 TeV. The analysis uses a data sample with an integrated luminosity of 139 fb$^{-1}$ collected by the ATLAS detector at the LHC from 2015 to 2018. The production cross-section for the process $pp \rightarrow \ell^+\ell^-\gamma+X$ ($\ell = e, \mu$) is measured within a fiducial phase-space region defined by kinematic requirements on the photon and the leptons, and by isolation requirements on the photon. An experimental precision of 2.9% is achieved for the fiducial cross-section. Differential cross-sections are measured as a function of each of six kinematic variables characterising the $\ell^+\ell^-\gamma$ system. The data are compared with theoretical predictions based on next-to-leading-order and next-to-next-to-leading-order perturbative QCD calculations. The impact of next-to-leading-order electroweak corrections is also considered. Journal of high energy physics 2020(3), 54 (2020). doi:10.1007/JHEP03(2020)054 Published by SISSA, [Trieste]

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  • Measurement of the $Z(\rightarrow\ell^+\ell^-)\gamma$ production cross-section in $pp$ collisions at $\sqrt{s} =13$ TeV with the ATLAS detector

    image/svg+xml art designer at PLoS, modified by Wikipedia users Nina, Beao, JakobVoss, and AnonMoos Open Access logo, converted into svg, designed by PLoS. This version with transparent background. http://commons.wikimedia.org/wiki/File:Open_Access_logo_PLoS_white.svg art designer at PLoS, modified by Wikipedia users Nina, Beao, JakobVoss, and AnonMoos http://www.plos.org/
    descriptionPublicationkeyboard_double_arrow_right Article , Research , Preprint 2019 Germany, France, Germany Publisher:Deutsches Elektronen-Synchrotron, DESY, Hamburg
    Authors: Aad, Georges; Abbott, Brad; Abreu, Henso; Araujo Pereira, Rodrigo; +196 Authors

    doi: 10.3204/pubdb-2020-02534 , 10.3204/pubdb-2019-05270

    arXiv: http://arxiv.org/abs/1911.04813 , 1911.04813

    The production of a prompt photon in association with a $Z$ boson is studied in proton-proton collisions at a centre-of-mass energy $\sqrt{s} =$ 13 TeV. The analysis uses a data sample with an integrated luminosity of 139 fb$^{-1}$ collected by the ATLAS detector at the LHC from 2015 to 2018. The production cross-section for the process $pp \rightarrow \ell^+\ell^-\gamma+X$ ($\ell = e, \mu$) is measured within a fiducial phase-space region defined by kinematic requirements on the photon and the leptons, and by isolation requirements on the photon. An experimental precision of 2.9% is achieved for the fiducial cross-section. Differential cross-sections are measured as a function of each of six kinematic variables characterising the $\ell^+\ell^-\gamma$ system. The data are compared with theoretical predictions based on next-to-leading-order and next-to-next-to-leading-order perturbative QCD calculations. The impact of next-to-leading-order electroweak corrections is also considered. Journal of high energy physics 2020(3), 54 (2020). doi:10.1007/JHEP03(2020)054 Published by SISSA, [Trieste]

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  • Measurement of isolated-photon plus two-jet production in pp collisions at $$ \sqrt{s} $$ = 13 TeV with the ATLAS detector

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    descriptionPublicationkeyboard_double_arrow_right Article , Preprint , Other literature type , Journal 2020Embargo end date: 01 Jan 2019 France, Netherlands, South Africa, United Kingdom, Italy, Poland, Italy, United Kingdom, Italy, Netherlands, Turkey, Italy, Spain, Portugal, Italy, Belarus, Netherlands, Norway, United Kingdom, Italy, Sweden, Germany, Italy, Spain, Germany, Turkey, Italy, Belarus, Netherlands, Czech Republic, China (People's Republic of), Italy, Italy, Italy, Italy, Chile, Czech Republic, Germany, Netherlands, China (People's Republic of), Spain, South Africa, Turkey, Norway, Germany, United Kingdom, China (People's Republic of), Italy, Australia, Denmark, Turkey, Australia, Australia, Italy, Italy, United States, Turkey Publisher:Springer Science and Business Media LLCFunded by:EC | PROBIST, GSRI
    Authors: Aad, Georges; Abbott, Brad; Abreu, Henso; Araujo Ferraz, Victor; +196 Authors

    doi: 10.1007/jhep03(2020)179 , 10.3204/pubdb-2020-02525 , 10.48550/arxiv.1912.09866 , 10.17863/cam.66468 , 10.17863/cam.53552 , 10.17863/cam.69498

    arXiv: 1912.09866 , http://arxiv.org/abs/1912.09866

    handle: 2066/218361 , https://repository.ubn.ru.nl/handle/2066/218361 , 11588/884357 , 11245.1/18bc9ce6-7e36-4673-bd77-df314f6020ed , 20.500.11851/9303 , 10852/83588 , 11250/2756168 , 10261/232887 , 10316/106311 , 10486/708879 , 10481/61851 , 20.500.11770/304198 , 11572/317931 , 11390/1182228 , 2108/275731 , 11590/388554 , 11573/1493191 , 11367/95123 , 11567/1103136 , 11568/1076219 , 11587/427313 , 11585/790275 , 1959.3/463676 , 11571/1370394 , 11343/252034 , 10210/463537 , 11411/2003

    Abstract The dynamics of isolated-photon plus two-jet production in pp collisions at a centre-of-mass energy of 13 TeV are studied with the ATLAS detector at the LHC using a dataset corresponding to an integrated luminosity of 36.1 fb−1. Cross sections are measured as functions of a variety of observables, including angular correlations and invariant masses of the objects in the final state, γ + jet + jet. Measurements are also performed in phase-space regions enriched in each of the two underlying physical mechanisms, namely direct and fragmentation processes. The measurements cover the range of photon (jet) transverse momenta from 150 GeV (100 GeV) to 2 TeV. The tree-level plus parton-shower predictions from Sherpa and Pythia as well as the next-to-leading-order QCD predictions from Sherpa are compared with the measurements. The next-to-leading-order QCD predictions describe the data adequately in shape and normalisation except for regions of phase space such as those with high values of the invariant mass or rapidity separation of the two jets, where the predictions overestimate the data.

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    CORE
    Article . 2020
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    Full-Text: https://eprints.gla.ac.uk/217121/1/217121.pdf
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    Article . 2020
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    Archivio istituzionale della ricerca - Università degli Studi di Udine
    Article . 2020
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    Full-Text: https://air.uniud.it/bitstream/11390/1182228/1/Aad2020_Article_MeasurementOfIsolated-photonPl.pdf
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    Archivio della Ricerca - Università di Roma Tor vergata
    Article . 2020
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    Full-Text: https://art.torvergata.it/bitstream/2108/275731/1/jhep.03.2020.179.pdf
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    Article . 2020
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    Archivio istituzionale della ricerca - Alma Mater Studiorum Università di Bologna
    Article . 2020
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    Journal of High Energy Physics
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    Full-Text: https://link.springer.com/content/pdf/10.1007/JHEP03(2020)179.pdf
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    University of Bergen: Bergen Open Research Archive (BORA-UiB)
    Article . 2020
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    Full-Text: https://hdl.handle.net/11250/2756168
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  • Measurement of isolated-photon plus two-jet production in pp collisions at $$ \sqrt{s} $$ = 13 TeV with the ATLAS detector

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    descriptionPublicationkeyboard_double_arrow_right Article , Preprint , Other literature type , Journal 2020Embargo end date: 01 Jan 2019 France, Netherlands, South Africa, United Kingdom, Italy, Poland, Italy, United Kingdom, Italy, Netherlands, Turkey, Italy, Spain, Portugal, Italy, Belarus, Netherlands, Norway, United Kingdom, Italy, Sweden, Germany, Italy, Spain, Germany, Turkey, Italy, Belarus, Netherlands, Czech Republic, China (People's Republic of), Italy, Italy, Italy, Italy, Chile, Czech Republic, Germany, Netherlands, China (People's Republic of), Spain, South Africa, Turkey, Norway, Germany, United Kingdom, China (People's Republic of), Italy, Australia, Denmark, Turkey, Australia, Australia, Italy, Italy, United States, Turkey Publisher:Springer Science and Business Media LLCFunded by:EC | PROBIST, GSRI
    Authors: Aad, Georges; Abbott, Brad; Abreu, Henso; Araujo Ferraz, Victor; +196 Authors

    doi: 10.1007/jhep03(2020)179 , 10.3204/pubdb-2020-02525 , 10.48550/arxiv.1912.09866 , 10.17863/cam.66468 , 10.17863/cam.53552 , 10.17863/cam.69498

    arXiv: 1912.09866 , http://arxiv.org/abs/1912.09866

    handle: 2066/218361 , https://repository.ubn.ru.nl/handle/2066/218361 , 11588/884357 , 11245.1/18bc9ce6-7e36-4673-bd77-df314f6020ed , 20.500.11851/9303 , 10852/83588 , 11250/2756168 , 10261/232887 , 10316/106311 , 10486/708879 , 10481/61851 , 20.500.11770/304198 , 11572/317931 , 11390/1182228 , 2108/275731 , 11590/388554 , 11573/1493191 , 11367/95123 , 11567/1103136 , 11568/1076219 , 11587/427313 , 11585/790275 , 1959.3/463676 , 11571/1370394 , 11343/252034 , 10210/463537 , 11411/2003

    Abstract The dynamics of isolated-photon plus two-jet production in pp collisions at a centre-of-mass energy of 13 TeV are studied with the ATLAS detector at the LHC using a dataset corresponding to an integrated luminosity of 36.1 fb−1. Cross sections are measured as functions of a variety of observables, including angular correlations and invariant masses of the objects in the final state, γ + jet + jet. Measurements are also performed in phase-space regions enriched in each of the two underlying physical mechanisms, namely direct and fragmentation processes. The measurements cover the range of photon (jet) transverse momenta from 150 GeV (100 GeV) to 2 TeV. The tree-level plus parton-shower predictions from Sherpa and Pythia as well as the next-to-leading-order QCD predictions from Sherpa are compared with the measurements. The next-to-leading-order QCD predictions describe the data adequately in shape and normalisation except for regions of phase space such as those with high values of the invariant mass or rapidity separation of the two jets, where the predictions overestimate the data.

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      Data sources: UnpayWall
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      Recolector de Ciencia Abierta, RECOLECTA
      2020
      License: CC BY
      Data sources: Recolector de Ciencia Abierta, RECOLECTA
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      Journal of High Energy Physics
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      TOBB ETU GCRIS Database
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  • Measurement of the $$t\bar{t}$$ production cross-section and lepton differential distributions in $$e\mu $$ dilepton events from pp collisions at $$\sqrt{s}=13\,\text {TeV}$$ with the ATLAS detector

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    descriptionPublicationkeyboard_double_arrow_right Article , Research , Preprint , Other literature type , Journal 2020Embargo end date: 01 Jan 2019 France, Switzerland, Turkey, China (People's Republic of), Italy, Australia, Netherlands, Italy, Norway, Netherlands, Italy, Italy, Turkey, Australia, Spain, United States, Norway, United Kingdom, Italy, Netherlands, Italy, Denmark, Italy, Italy, Sweden, Germany, United Kingdom, Netherlands, Italy, Spain, Germany, Portugal, China (People's Republic of), Australia, Italy, Italy, Netherlands, Czech Republic, Turkey, Spain, Chile, Italy, China (People's Republic of), Turkey, Czech Republic, Poland, United Kingdom, Italy, Italy, United Kingdom, Italy, Germany Publisher:Springer Science and Business Media LLCFunded by:EC | PROBIST
    Authors: Aad, Georges; Abbott, Brad; Abreu, Henso; Arcangeletti, Chiara; +196 Authors

    doi: 10.1140/epjc/s10052-020-7907-9 , 10.48550/arxiv.1910.08819 , 10.3204/pubdb-2019-05253 , 10.17863/cam.54305 , 10.17863/cam.56336 , 10.17863/cam.53878 , 10.17863/cam.71238 , 10.3204/pubdb-2020-02552 , 10.17863/cam.55182

    arXiv: 1910.08819 , http://arxiv.org/abs/1910.08819

    handle: 2066/221204 , 2066/221923 , https://repository.ubn.ru.nl/handle/2066/221204 , 11588/884416 , 11245.1/63948321-7440-4575-bbe9-d7fcb633bb42 , 20.500.11851/9777 , 11250/2755506 , 10852/83795 , 10261/232448 , 10316/106040 , 10486/704298 , 10481/64525 , 20.500.11770/306706 , 11572/318659 , 11390/1187851 , 2108/275805 , 11590/388717 , 11573/1494293 , 11367/95174 , 11567/1034593 , 11568/1075979 , 11587/439702 , 11585/783052 , 11343/252094 , 11571/1370850 , 1959.3/463769

    AbstractThe inclusive top quark pair ($$t\bar{t}$$ t t ¯ ) production cross-section $$\sigma _{t\bar{t}}$$ σ t t ¯ has been measured in proton–proton collisions at $$\sqrt{s}=13\,\text {TeV}$$ s = 13 TeV , using 36.1 fb$$^{-1}$$ - 1 of data collected in 2015–2016 by the ATLAS experiment at the LHC. Using events with an opposite-charge $$e\mu $$ e μ pair and b-tagged jets, the cross-section is measured to be: $$\begin{aligned} \sigma _{t\bar{t}} = 826.4 \pm 3.6\,\mathrm {(stat)}\ \pm 11.5\,\mathrm {(syst)}\ \pm 15.7\,\mathrm {(lumi)}\ \pm 1.9\,\mathrm {(beam)}\,\mathrm {pb}, \end{aligned}$$ σ t t ¯ = 826.4 ± 3.6 ( stat ) ± 11.5 ( syst ) ± 15.7 ( lumi ) ± 1.9 ( beam ) pb , where the uncertainties reflect the limited size of the data sample, experimental and theoretical systematic effects, the integrated luminosity, and the LHC beam energy, giving a total uncertainty of 2.4%. The result is consistent with theoretical QCD calculations at next-to-next-to-leading order. It is used to determine the top quark pole mass via the dependence of the predicted cross-section on $$m_t^{\mathrm{pole}}$$ m t pole , giving $$m_t^{\mathrm{pole}}=173.1^{+2.0}_{-2.1}\,\text {GeV}$$ m t pole = 173 . 1 - 2.1 + 2.0 GeV . It is also combined with measurements at $$\sqrt{s}=7\,\text {TeV}$$ s = 7 TeV and $$\sqrt{s}=8\,\text {TeV}$$ s = 8 TeV to derive ratios and double ratios of $$t\bar{t}$$ t t ¯ and Z cross-sections at different energies. The same event sample is used to measure absolute and normalised differential cross-sections as functions of single-lepton and dilepton kinematic variables, and the results are compared with predictions from various Monte Carlo event generators.

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      Recolector de Ciencia Abierta, RECOLECTA
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      European Physical Journal C: Particles and Fields
      Journal
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      Publikationer från Uppsala Universitet
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      Digitala Vetenskapliga Arkivet - Academic Archive On-line
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  • Measurement of the $$t\bar{t}$$ production cross-section and lepton differential distributions in $$e\mu $$ dilepton events from pp collisions at $$\sqrt{s}=13\,\text {TeV}$$ with the ATLAS detector

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    descriptionPublicationkeyboard_double_arrow_right Article , Research , Preprint , Other literature type , Journal 2020Embargo end date: 01 Jan 2019 France, Switzerland, Turkey, China (People's Republic of), Italy, Australia, Netherlands, Italy, Norway, Netherlands, Italy, Italy, Turkey, Australia, Spain, United States, Norway, United Kingdom, Italy, Netherlands, Italy, Denmark, Italy, Italy, Sweden, Germany, United Kingdom, Netherlands, Italy, Spain, Germany, Portugal, China (People's Republic of), Australia, Italy, Italy, Netherlands, Czech Republic, Turkey, Spain, Chile, Italy, China (People's Republic of), Turkey, Czech Republic, Poland, United Kingdom, Italy, Italy, United Kingdom, Italy, Germany Publisher:Springer Science and Business Media LLCFunded by:EC | PROBIST
    Authors: Aad, Georges; Abbott, Brad; Abreu, Henso; Arcangeletti, Chiara; +196 Authors

    doi: 10.1140/epjc/s10052-020-7907-9 , 10.48550/arxiv.1910.08819 , 10.3204/pubdb-2019-05253 , 10.17863/cam.54305 , 10.17863/cam.56336 , 10.17863/cam.53878 , 10.17863/cam.71238 , 10.3204/pubdb-2020-02552 , 10.17863/cam.55182

    arXiv: 1910.08819 , http://arxiv.org/abs/1910.08819

    handle: 2066/221204 , 2066/221923 , https://repository.ubn.ru.nl/handle/2066/221204 , 11588/884416 , 11245.1/63948321-7440-4575-bbe9-d7fcb633bb42 , 20.500.11851/9777 , 11250/2755506 , 10852/83795 , 10261/232448 , 10316/106040 , 10486/704298 , 10481/64525 , 20.500.11770/306706 , 11572/318659 , 11390/1187851 , 2108/275805 , 11590/388717 , 11573/1494293 , 11367/95174 , 11567/1034593 , 11568/1075979 , 11587/439702 , 11585/783052 , 11343/252094 , 11571/1370850 , 1959.3/463769

    AbstractThe inclusive top quark pair ($$t\bar{t}$$ t t ¯ ) production cross-section $$\sigma _{t\bar{t}}$$ σ t t ¯ has been measured in proton–proton collisions at $$\sqrt{s}=13\,\text {TeV}$$ s = 13 TeV , using 36.1 fb$$^{-1}$$ - 1 of data collected in 2015–2016 by the ATLAS experiment at the LHC. Using events with an opposite-charge $$e\mu $$ e μ pair and b-tagged jets, the cross-section is measured to be: $$\begin{aligned} \sigma _{t\bar{t}} = 826.4 \pm 3.6\,\mathrm {(stat)}\ \pm 11.5\,\mathrm {(syst)}\ \pm 15.7\,\mathrm {(lumi)}\ \pm 1.9\,\mathrm {(beam)}\,\mathrm {pb}, \end{aligned}$$ σ t t ¯ = 826.4 ± 3.6 ( stat ) ± 11.5 ( syst ) ± 15.7 ( lumi ) ± 1.9 ( beam ) pb , where the uncertainties reflect the limited size of the data sample, experimental and theoretical systematic effects, the integrated luminosity, and the LHC beam energy, giving a total uncertainty of 2.4%. The result is consistent with theoretical QCD calculations at next-to-next-to-leading order. It is used to determine the top quark pole mass via the dependence of the predicted cross-section on $$m_t^{\mathrm{pole}}$$ m t pole , giving $$m_t^{\mathrm{pole}}=173.1^{+2.0}_{-2.1}\,\text {GeV}$$ m t pole = 173 . 1 - 2.1 + 2.0 GeV . It is also combined with measurements at $$\sqrt{s}=7\,\text {TeV}$$ s = 7 TeV and $$\sqrt{s}=8\,\text {TeV}$$ s = 8 TeV to derive ratios and double ratios of $$t\bar{t}$$ t t ¯ and Z cross-sections at different energies. The same event sample is used to measure absolute and normalised differential cross-sections as functions of single-lepton and dilepton kinematic variables, and the results are compared with predictions from various Monte Carlo event generators.

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      European Physical Journal C: Particles and Fields
      Article
      License: CC BY
      Full-Text: https://link.springer.com/content/pdf/10.1140/epjc/s10052-020-7907-9.pdf
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      Full-Text: https://qmro.qmul.ac.uk/xmlui/handle/123456789/66073
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      Full-Text: https://hdl.handle.net/11250/2755506
      Data sources: Bielefeld Academic Search Engine (BASE)
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      Data sources: UnpayWall
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      Recolector de Ciencia Abierta, RECOLECTA
      2020
      License: CC BY
      Data sources: Recolector de Ciencia Abierta, RECOLECTA
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      European Physical Journal C: Particles and Fields
      Journal
      Data sources: Microsoft Academic Graph
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      Norwegian Open Research Archives
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      Publikationer från Uppsala Universitet
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      Digitala Vetenskapliga Arkivet - Academic Archive On-line
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      Bergen Open Research Archive - UiB
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      European Physical Journal C: Particles and Fields
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      TOBB ETU GCRIS Database
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  • Measurement of the cross section for isolated-photon plus jet production in $pp$ collisions at $\sqrt s=13$ TeV using the ATLAS detector

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    descriptionPublicationkeyboard_double_arrow_right Article , Research , Preprint , Journal , Other literature type 2017Embargo end date: 01 Jan 2018 Italy, Italy, Turkey, Germany, France, United Kingdom, Italy, United Kingdom, Germany, Germany, South Africa, South Africa, Italy, Turkey, United Kingdom, United Kingdom, United Kingdom, Italy, Switzerland, Italy, United Kingdom, United Kingdom, Italy, Italy, Italy, Italy Publisher:arXivFunded by:GSRI
    Authors: Jeannine Wagner-kuhr; Juraj Bracinik; Yoichi Ninomiya; Pavel Starovoitov; +196 Authors

    doi: 10.48550/arxiv.1801.00112 , 10.3204/pubdb-2018-00059 , 10.3204/pubdb-2018-01922

    arXiv: http://arxiv.org/abs/1801.00112 , 1801.00112

    handle: 2434/587256 , 20.500.11770/304349 , 11390/1131440 , 2108/200863 , 11590/337685 , 11573/1216320 , 11367/72188 , 11568/947245 , 11568/1164402 , 11571/1271006 , 10210/287612

    The dynamics of isolated-photon production in association with a jet in proton–proton collisions at a centre-of-mass energy of 13 TeV are studied with the ATLAS detector at the LHC using a dataset with an integrated luminosity of 3.2 $fb^{−1}$. Photons are required to have transverse energies above 125 GeV. Jets are identified using the anti-$k_t$ algorithm with radius parameter $R = 0.4$ and required to have transverse momenta above 100 GeV. Measurements of isolated-photon plus jet cross sections are presented as functions of the leading-photon transverse energy, the leading-jet transverse momentum, the azimuthal angular separation between the photon and the jet, the photon–jet invariant mass and the scattering angle in the photon–jet centre-of-mass system. Tree-level plus parton-shower predictions from Sherpa and Pythia as well as next-to-leading-order QCD predictions from Jetphox and Sherpa are compared to the measurements. Physics letters / B 780, 578 - 602 (2018). doi:10.1016/j.physletb.2018.03.035 Published by North-Holland Publ., Amsterdam

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  • Measurement of the cross section for isolated-photon plus jet production in $pp$ collisions at $\sqrt s=13$ TeV using the ATLAS detector

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    descriptionPublicationkeyboard_double_arrow_right Article , Research , Preprint , Journal , Other literature type 2017Embargo end date: 01 Jan 2018 Italy, Italy, Turkey, Germany, France, United Kingdom, Italy, United Kingdom, Germany, Germany, South Africa, South Africa, Italy, Turkey, United Kingdom, United Kingdom, United Kingdom, Italy, Switzerland, Italy, United Kingdom, United Kingdom, Italy, Italy, Italy, Italy Publisher:arXivFunded by:GSRI
    Authors: Jeannine Wagner-kuhr; Juraj Bracinik; Yoichi Ninomiya; Pavel Starovoitov; +196 Authors

    doi: 10.48550/arxiv.1801.00112 , 10.3204/pubdb-2018-00059 , 10.3204/pubdb-2018-01922

    arXiv: http://arxiv.org/abs/1801.00112 , 1801.00112

    handle: 2434/587256 , 20.500.11770/304349 , 11390/1131440 , 2108/200863 , 11590/337685 , 11573/1216320 , 11367/72188 , 11568/947245 , 11568/1164402 , 11571/1271006 , 10210/287612

    The dynamics of isolated-photon production in association with a jet in proton–proton collisions at a centre-of-mass energy of 13 TeV are studied with the ATLAS detector at the LHC using a dataset with an integrated luminosity of 3.2 $fb^{−1}$. Photons are required to have transverse energies above 125 GeV. Jets are identified using the anti-$k_t$ algorithm with radius parameter $R = 0.4$ and required to have transverse momenta above 100 GeV. Measurements of isolated-photon plus jet cross sections are presented as functions of the leading-photon transverse energy, the leading-jet transverse momentum, the azimuthal angular separation between the photon and the jet, the photon–jet invariant mass and the scattering angle in the photon–jet centre-of-mass system. Tree-level plus parton-shower predictions from Sherpa and Pythia as well as next-to-leading-order QCD predictions from Jetphox and Sherpa are compared to the measurements. Physics letters / B 780, 578 - 602 (2018). doi:10.1016/j.physletb.2018.03.035 Published by North-Holland Publ., Amsterdam

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  • The energy spectrum of cosmic rays beyond the turn-down around $$\varvec{10^{17}}$$ eV as measured with the surface detector of the Pierre Auger Observatory

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    descriptionPublicationkeyboard_double_arrow_right Article , Research , Preprint , Journal 2021Embargo end date: 01 Jan 2021 Netherlands, Italy, Slovenia, Netherlands, Spain, Czech Republic, Italy, Italy, Italy, Argentina, Netherlands, Netherlands, France, Italy, Germany, Czech Republic, Belgium, Italy, Argentina, Italy, Germany, Netherlands Publisher:Springer Science and Business Media LLCFunded by:NSF | Pierre Auger Project, ANR | SUPER
    Authors: G. Medina-Tanco; J. Stasielak; G. Farrar; Trent D. Grubb; +196 Authors

    doi: 10.1140/epjc/s10052-021-09700-w , 10.48550/arxiv.2109.13400 , 10.18154/rwth-2021-12100 , 10.18154/rwth-2022-00047

    arXiv: http://arxiv.org/abs/2109.13400 , 2109.13400

    handle: https://repository.ubn.ru.nl/handle/2066/239867 , 11588/890384 , 11245.1/e277820a-6074-4fdc-9cd2-9d87842d0efe , 2066/239867 , 2434/1033134 , 10481/71942 , 20.500.12556/RUNG-6965 , 11311/1189557 , 20.500.14017/fb76dc10-e5e8-4ff6-88c2-75af44762dfb , 11697/176134 , 11587/458363 , 20.500.11769/526705 , 2318/1841975 , 2133/23683

    AbstractWe present a measurement of the cosmic-ray spectrum above 100 PeV using the part of the surface detector of the Pierre Auger Observatory that has a spacing of 750 m. An inflection of the spectrum is observed, confirming the presence of the so-called second-knee feature. The spectrum is then combined with that of the 1500 m array to produce a single measurement of the flux, linking this spectral feature with the three additional breaks at the highest energies. The combined spectrum, with an energy scale set calorimetrically via fluorescence telescopes and using a single detector type, results in the most statistically and systematically precise measurement of spectral breaks yet obtained. These measurements are critical for furthering our understanding of the highest energy cosmic rays.

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  • The energy spectrum of cosmic rays beyond the turn-down around $$\varvec{10^{17}}$$ eV as measured with the surface detector of the Pierre Auger Observatory

    image/svg+xml art designer at PLoS, modified by Wikipedia users Nina, Beao, JakobVoss, and AnonMoos Open Access logo, converted into svg, designed by PLoS. This version with transparent background. http://commons.wikimedia.org/wiki/File:Open_Access_logo_PLoS_white.svg art designer at PLoS, modified by Wikipedia users Nina, Beao, JakobVoss, and AnonMoos http://www.plos.org/
    descriptionPublicationkeyboard_double_arrow_right Article , Research , Preprint , Journal 2021Embargo end date: 01 Jan 2021 Netherlands, Italy, Slovenia, Netherlands, Spain, Czech Republic, Italy, Italy, Italy, Argentina, Netherlands, Netherlands, France, Italy, Germany, Czech Republic, Belgium, Italy, Argentina, Italy, Germany, Netherlands Publisher:Springer Science and Business Media LLCFunded by:NSF | Pierre Auger Project, ANR | SUPER
    Authors: G. Medina-Tanco; J. Stasielak; G. Farrar; Trent D. Grubb; +196 Authors

    doi: 10.1140/epjc/s10052-021-09700-w , 10.48550/arxiv.2109.13400 , 10.18154/rwth-2021-12100 , 10.18154/rwth-2022-00047

    arXiv: http://arxiv.org/abs/2109.13400 , 2109.13400

    handle: https://repository.ubn.ru.nl/handle/2066/239867 , 11588/890384 , 11245.1/e277820a-6074-4fdc-9cd2-9d87842d0efe , 2066/239867 , 2434/1033134 , 10481/71942 , 20.500.12556/RUNG-6965 , 11311/1189557 , 20.500.14017/fb76dc10-e5e8-4ff6-88c2-75af44762dfb , 11697/176134 , 11587/458363 , 20.500.11769/526705 , 2318/1841975 , 2133/23683

    AbstractWe present a measurement of the cosmic-ray spectrum above 100 PeV using the part of the surface detector of the Pierre Auger Observatory that has a spacing of 750 m. An inflection of the spectrum is observed, confirming the presence of the so-called second-knee feature. The spectrum is then combined with that of the 1500 m array to produce a single measurement of the flux, linking this spectral feature with the three additional breaks at the highest energies. The combined spectrum, with an energy scale set calorimetrically via fluorescence telescopes and using a single detector type, results in the most statistically and systematically precise measurement of spectral breaks yet obtained. These measurements are critical for furthering our understanding of the highest energy cosmic rays.

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  • Measurement of the $Z(\rightarrow\ell^+\ell^-)\gamma$ production cross-section in $pp$ collisions at $\sqrt{s} =13$ TeV with the ATLAS detector

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    descriptionPublicationkeyboard_double_arrow_right Article , Research , Preprint 2019 Germany, France, Germany Publisher:Deutsches Elektronen-Synchrotron, DESY, Hamburg
    Authors: Aad, Georges; Abbott, Brad; Abreu, Henso; Araujo Pereira, Rodrigo; +196 Authors

    doi: 10.3204/pubdb-2020-02534 , 10.3204/pubdb-2019-05270

    arXiv: http://arxiv.org/abs/1911.04813 , 1911.04813

    The production of a prompt photon in association with a $Z$ boson is studied in proton-proton collisions at a centre-of-mass energy $\sqrt{s} =$ 13 TeV. The analysis uses a data sample with an integrated luminosity of 139 fb$^{-1}$ collected by the ATLAS detector at the LHC from 2015 to 2018. The production cross-section for the process $pp \rightarrow \ell^+\ell^-\gamma+X$ ($\ell = e, \mu$) is measured within a fiducial phase-space region defined by kinematic requirements on the photon and the leptons, and by isolation requirements on the photon. An experimental precision of 2.9% is achieved for the fiducial cross-section. Differential cross-sections are measured as a function of each of six kinematic variables characterising the $\ell^+\ell^-\gamma$ system. The data are compared with theoretical predictions based on next-to-leading-order and next-to-next-to-leading-order perturbative QCD calculations. The impact of next-to-leading-order electroweak corrections is also considered. Journal of high energy physics 2020(3), 54 (2020). doi:10.1007/JHEP03(2020)054 Published by SISSA, [Trieste]

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  • Measurement of the $Z(\rightarrow\ell^+\ell^-)\gamma$ production cross-section in $pp$ collisions at $\sqrt{s} =13$ TeV with the ATLAS detector

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    descriptionPublicationkeyboard_double_arrow_right Article , Research , Preprint 2019 Germany, France, Germany Publisher:Deutsches Elektronen-Synchrotron, DESY, Hamburg
    Authors: Aad, Georges; Abbott, Brad; Abreu, Henso; Araujo Pereira, Rodrigo; +196 Authors

    doi: 10.3204/pubdb-2020-02534 , 10.3204/pubdb-2019-05270

    arXiv: http://arxiv.org/abs/1911.04813 , 1911.04813

    The production of a prompt photon in association with a $Z$ boson is studied in proton-proton collisions at a centre-of-mass energy $\sqrt{s} =$ 13 TeV. The analysis uses a data sample with an integrated luminosity of 139 fb$^{-1}$ collected by the ATLAS detector at the LHC from 2015 to 2018. The production cross-section for the process $pp \rightarrow \ell^+\ell^-\gamma+X$ ($\ell = e, \mu$) is measured within a fiducial phase-space region defined by kinematic requirements on the photon and the leptons, and by isolation requirements on the photon. An experimental precision of 2.9% is achieved for the fiducial cross-section. Differential cross-sections are measured as a function of each of six kinematic variables characterising the $\ell^+\ell^-\gamma$ system. The data are compared with theoretical predictions based on next-to-leading-order and next-to-next-to-leading-order perturbative QCD calculations. The impact of next-to-leading-order electroweak corrections is also considered. Journal of high energy physics 2020(3), 54 (2020). doi:10.1007/JHEP03(2020)054 Published by SISSA, [Trieste]

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