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New Facilities for the Production of 1 mm gap Resistive Plate Chambers for the Upgrade of the ATLAS Muon Spectrometer / Fallavollita, F. (Auckland U.) ; Kortner, O. (Auckland U.) ; Kroha, H. (Auckland U.) ; Maly, P. (Auckland U.) ; Proto, G. (Auckland U.) ; Soyk, D. (Auckland U.) ; Voevodina, E. ; Zimmermann, J. (Auckland U.)
The ATLAS Muon Spectrometer is undergoing a major upgrade for the High-Luminosity LHC (HL-LHC), including the addition of three new thin-gap Resistive Plate Chamber (RPC) layers in the inner barrel region. [...]
arXiv:2501.04756. - 27.
Fulltext

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The ATLAS experiment at the CERN Large Hadron Collider: a description of the detector configuration for Run 3 / ATLAS Collaboration
The ATLAS detector is installed in its experimental cavern at Point 1 of the CERN Large Hadron Collider. During Run 2 of the LHC, a luminosity of $\mathcal{L}=2\times 10^{34}\mathrm{cm}^{-2}\mathrm{s}^{-1}$ was routinely achieved at the start of fills, twice the design luminosity. [...]
arXiv:2305.16623; CERN-EP-2022-259.- Geneva : CERN, 2024-05-23 - 233 p. - Published in : JINST 19 (2024) P05063 Fulltext: ANA-GENR-2019-02-PAPER - PDF; 2305.16623 - PDF; document - PDF; External link: Previous draft version
In : The Large Hadron Collider and The Experiments for Run 3

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Commissioning and Installation of the New small-Diameter Muon Drift Tube (sMDT) Detectors for the Phase-I Upgrade of the ATLAS Muon Spectrometer / Eberwein, G.H. (Munich, Max Planck Inst.) ; Kortner, O. (Munich, Max Planck Inst.) ; Kroha, H. (Munich, Max Planck Inst.) ; Rendel, M. (Munich, Max Planck Inst.) ; Rieck, P. (Munich, Max Planck Inst.) ; Soyk, D. (Munich, Max Planck Inst.) ; Voevodina, E. (Munich, Max Planck Inst.) ; Walbrecht, V. (Munich, Max Planck Inst.) /ATLAS Muon Group Collaboration
The Monitored Drift Tubes, as a part of the ATLAS muon spectrometer, are precision drift chambers designed to provide excellent spatial resolution and high tracking efficiency independent of the track angle. Through the life of the LHC and ATLAS experiment, this detector has already demonstrated that they provide precise tracking over large areas. [...]
arXiv:2112.07026.- 2021-10-16 - 4 p. - Published in : 10.1109/NSS/MIC44867.2021.9875793 Fulltext: PDF;
In : IEEE NSS MIC 2021, Online, Japan, 16 - 23 Oct 2021, pp.1-4

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Production of pions, kaons and protons in pp collisions at $\sqrt{s}$ = 900 GeV with ALICE at the LHC / ALICE Collaboration
The production of $\pi^+, pi^-, K^+, K^-$, p, and $\bar{p}$ at mid-rapidity has been measured in proton-proton collisions at $\sqrt{s}$ = 900 GeV with the ALICE detector. Particle identification is performed using the specific energy loss in the inner tracking silicon detector and the time projection chamber. [...]
arXiv:1101.4110; CERN-PH-EP-2010-085; CERN-PH-EP-2010-085.- Geneva : CERN, 2011 - 30 p. - Published in : Eur. Phys. J. C 71 (2011) 1655 Author list: TEX; Fulltext: PDF; Springer Open Access article: PDF; External link: Rivet analyses reference

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Transverse momentum spectra of charged particles in proton-proton collisions at $\sqrt{s}$ = 900 GeV with ALICE at the LHC / ALICE Collaboration
The inclusive charged particle transverse momentum distribution is measured in proton-proton collisions at $\sqrt{s} = 900$~GeV at the LHC using the ALICE detector. The measurement is performed in the central pseudorapidity region $(|\eta|<0.8)$ over the transverse momentum range $0.15_{\rm INEL}=0.483\pm0.001$~(stat.)~$\pm0.007$~(syst.)~GeV/$c$ and $\left_{\rm NSD}=0.489\pm0.001$~(stat.)~$\pm0.007$~(syst.)~GeV/$c$, respectively. [...]
arXiv:1007.0719.- 2010 - 20 p. - Published in : Phys. Lett. B 693 (2010) 53-68 Elsevier Open Access article: PDF; Fulltext: PDF; External link: Rivet analyses reference

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Two-pion Bose-Einstein correlations in $pp$ collisions at $\sqrt{s}$=900 GeV / ALICE Collaboration
We report on the measurement of two-pion correlation functions from pp collisions at sqrt(s)=900 GeV performed by the ALICE experiment at the Large Hadron Collider. Our analysis shows an increase of the HBT radius with increasing event multiplicity, in line with other measurements done in particle- and nuclear collisions. [...]
arXiv:1007.0516.- 2010 - 13 p. - Published in : Phys. Rev. D 82 (2010) 052001 APS Open Access article: PDF; Fulltext: PDF; External link: DURHAM

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Midrapidity antiproton-to-proton ratio in pp collisions at $\sqrt{s} = 0.9$ and $7$~TeV measured by the ALICE experiment / ALICE collaboration
The ratio of the yields of antiprotons to protons in pp collisions has been measured by the ALICE experiment at $\sqrt{s} = 0.9$ and $7$~TeV during the initial running periods of the Large Hadron Collider(LHC). The measurement covers the transverse momentum interval $0.45 < p_{\rm{t}} < 1.05$~GeV/$c$ and rapidity $|y| < 0.5$. [...]
arXiv:1006.5432.- 2010 - 12 p. - Published in : Phys. Rev. Lett. 105 (2010) 072002 APS Open Access article: PDF; Fulltext: PDF; External link: DURHAM

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Charged-particle multiplicity measurement in proton-proton collisions at $\sqrt{s}$ = 7 TeV with ALICE at LHC / ALICE Collaboration
The pseudorapidity density and multiplicity distribution of charged particles produced in proton-proton collisions at the LHC, at a centre-of-mass energy sqrt(s) = 7 TeV, were measured in the central pseudorapidity region |eta| < 1. Comparisons are made with previous measurements at sqrt(s) = 0.9 TeV and 2.36 TeV. [...]
arXiv:1004.3514.- 2010 - 11 p. - Published in : Eur. Phys. J. C 68 (2010) 345-354 Fulltext: 10052_2010_1350_OnlinePDF - PDF; arXiv:1004.3514 - PDF; Springer Open Access article: PDF; External link: Rivet analyses reference

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Charged-particle multiplicity measurement in proton-proton collisions at $\sqrt{s}$ = 0.9 and 2.36 TeV with ALICE at LHC / ALICE Collaboration
Charged-particle production was studied in proton-proton collisions collected at the LHC with the ALICE detector at centre-of-mass energies 0.9 TeV and 2.36 TeV in the pseudorapidity range |eta| < 1.4. In the central region (|eta| < 0.5), at 0.9 TeV, we measure charged-particle pseudorapidity density dNch/deta = 3.02 +- 0.01 (stat.) +0.08 -0.05 (syst.) for inelastic interactions, and dNch/deta = 3.58 +- 0.01 (stat.) +0.12 -0.12 (syst.) for non-single-diffractive interactions. [...]
arXiv:1004.3034.- 2010 - 20 p. - Published in : Eur. Phys. J. C 68 (2010) 89-108 Fulltext: arXiv:1004.3034 - PDF; 10052_2010_1339_OnlinePDF - PDF; Springer Open Access article: PDF; External link: Rivet analyses reference

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10.

The ALICE TPC, a large 3-dimensional tracking device with fast readout for ultra-high multiplicity events / Alme, J. (Bergen U.) ; Andres, Y. (CERN) ; Appelshauser, H. (Frankfurt U., FIAS) ; Bablok, S. (Bergen U.) ; Bialas, N. (Bergen U.) ; Bolgen, R. (Bergen U.) ; Bonnes, U. (Darmstadt, Tech. Hochsch.) ; Bramm, R. (Darmstadt, GSI) ; Braun-Munzinger, P. (Darmstadt, Tech. Hochsch. ; Darmstadt, GSI ; Darmstadt, EMMI ; Frankfurt U., Inst. Kernphys.) ; Campagnolo, R. (CERN) et al.
The design, construction, and commissioning of the ALICE Time-Projection Chamber (TPC) is described. It is the main device for pattern recognition, tracking, and identification of charged particles in the ALICE experiment at the CERN LHC. [...]
arXiv:1001.1950.- 2010 - 56 p. - Published in : Nucl. Instrum. Methods Phys. Res., A 622 (2010) 316-367 Fulltext: PDF; External link: Preprint

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8	Soyk, D.
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