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Charged-hadron and identified-hadron ( $K^\mathrm{0}_\mathrm{S}$ , $\Lambda$ , $\Xi^\mathrm{-}$ ) yield measurements in photo-nuclear Pb+Pb and $p$ +Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV with ATLAS / ATLAS Collaboration
This paper presents the measurement of charged-hadron and identified-hadron (

$K^\mathrm{0}_\mathrm{S}$ ,

$\Lambda$ ,

$\Xi^\mathrm{-}$ ) yields in photo-nuclear collisions using 1.7

$\mathrm{nb^{-1}}$ of

$\sqrt{s_\mathrm{NN}} = 5.02$ TeV Pb+Pb data collected in 2018 with the ATLAS detector at the Large Hadron Collider. [...]
arXiv:2503.08181 ; CERN-EP-2025-040. - 2025 - 51.
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ITk pixel system test of the ATLAS experiment / Chubinidze, Zaza (Frascati) /ATLAS Collaboration
The ATLAS experiment is preparing for the High-Luminosity LHC (HL-LHC) upgrade, which will require the substitution of the current Inner Detector (ID) with a new all-silicon Inner Tracker (ITk). This work presents the results of the ITk Pixel system test, focusing on module performance, power consumption, data transmission and cooling efficiency, during detector integration. [...]
2025 - 8 p. - Published in : JINST
Fulltext: PDF;
In : 25th international Workshop on Radiation Imaging Detectors (iWoRiD2024), Lisbon, Portugal, 30 Jun - 4 Jul 2024, pp.C02038

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Measurement of double-differential charged-current Drell-Yan cross-sections at high transverse masses in $pp$ collisions at $\sqrt{s} =$ 13 TeV with the ATLAS detector / ATLAS Collaboration
This paper presents a first measurement of the cross-section for the charged-current Drell-Yan process

$pp\rightarrow W^{\pm} \rightarrow \ell^{\pm} \nu$ above the resonance region, where

$\ell$ is an electron or muon [...]
CERN-EP-2025-032 ; arXiv:2502.21088. - 64.
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Measurement of the top quark mass with the ATLAS detector using $t\bar{t}$ events with a high transverse momentum top quark / ATLAS Collaboration
The mass of the top quark is measured using top-antitop-quark pair events with high transverse momentum top quarks. [...]
arXiv:2502.18216 ; CERN-EP-2025-015. - 2025 - 43.
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Weakly supervised anomaly detection for resonant new physics in the dijet final state using proton-proton collisions at $\sqrt{s}=13$ TeV with the ATLAS detector / ATLAS Collaboration
An anomaly detection search for narrow-width resonances beyond the Standard Model that decay into a pair of jets is presented. [...]
arXiv:2502.09770 ; CERN-EP-2025-002. - 2025 - 50.
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Measurement of $W^{\pm}$ -boson differential cross-sections in proton-proton collisions with low pile-up data at $\sqrt{s} = 5.02$ TeV and $13$ TeV with the ATLAS detector / ATLAS Collaboration
High precision single-differential

$W^\pm$ -boson production cross-sections as a function of electron or muon transverse momentum

$p_\mathrm{T}$ or their pseudorapity

$\eta$ , as well as double-differential cross-sections as functions of these variables, are measured in proton-proton collisions at centre-of-mass energies

$\sqrt{s}=5.02$ TeV and 13 TeV. [...]
arXiv:2502.09403 ; CERN-EP-2025-009. - 2025 - 45.
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Search for long-lived charged particles using large specific ionisation loss and time of flight in 140 fb $^{-1}$ of $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector / ATLAS Collaboration
This paper presents a search for massive, charged, long-lived particles with the ATLAS detector at the Large Hadron Collider using an integrated luminosity of 140 fb

$^{-1}$ of proton-proton collisions at

$\sqrt{s}=13$ TeV. [...]
arXiv:2502.06694 ; CERN-EP-2025-008. - 2025 - 56.
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Estimation of backgrounds from jets misidentified as $\tau$ -leptons using the Universal Fake Factor method with the ATLAS detector / ATLAS Collaboration
Processes with

$\tau$ -leptons in the final state are important for Standard Model measurements and searches for physics beyond the Standard Model. [...]
arXiv:2502.04156 ; CERN-EP-2025-003. - 2025 - 47.
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Measurement of jet track functions in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector / ATLAS Collaboration
Measurements of jet substructure are key to probing the energy frontier at colliders, and many of them use track-based observables which take advantage of the angular precision of tracking detectors. [...]
arXiv:2502.02062 ; CERN-EP-2024-333. - 2025 - 36.
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10.

Configuration, Performance, and Commissioning of the ATLAS $b$ -jet Triggers for the 2022 and 2023 LHC data-taking periods / ATLAS Collaboration
In 2022 and 2023, the Large Hadron Collider produced approximately two billion hadronic interactions each second from bunches of protons that collide at a rate of 40 MHz. The ATLAS trigger system is used to reduce this rate to a few kHz for recording. [...]
arXiv:2501.11420; CERN-EP-2025-004.- Geneva : CERN, 2025-03-04 - 47 p. - Published in : JINST 20 (2025) P03002 Fulltext: ANA-TRIG-2022-02-PAPER - PDF; 2501.11420 - PDF; document - PDF; External link: Previous draft version

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2	Chubinidze, Z

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