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The ALICE experiment: a journey through QCD / ALICE Collaboration
The ALICE experiment was proposed in 1993, to study strongly interacting matter at extreme energy densities via a comprehensive investigation of nuclear collisions at the LHC. Its physics programme initially focused on the determination of the properties of the Quark-Gluon Plasma (QGP), a deconfined state of quarks and gluons and was extended along the years, covering a diverse ensemble of observables related to Quantum Chromodynamics (QCD), the theory of strong interactions. [...]
arXiv:2211.04384; CERN-EP-2022-227.- Geneva : CERN, 2024-08-14 - 221 p. - Published in : Eur. Phys. J. C 84 (2024) 813 Draft (restricted): PDF; Fulltext: 2211.04384 - PDF; document - PDF;

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Performance of the ALICE Electromagnetic Calorimeter / ALICE Collaboration
The performance of the electromagnetic calorimeter of the ALICE experiment during operation in 2010$-$2018 at the Large Hadron Collider is presented. After a short introduction into the design, readout, and trigger capabilities of the detector, the procedures for data taking, reconstruction, and validation are explained. [...]
arXiv:2209.04216; CERN-EP-2022-184.- Geneva : CERN, 2023-08-10 - 139 p. - Published in : JINST 18 (2023) P08007 Draft (restricted): PDF; Fulltext: 2209.04216 - PDF; document - PDF;

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Evolution of jet shapes and fragmentation functions in Au+Au collisions at $\sqrt{s_\mathrm{NN}}=200$ GeV with the STAR experiment at RHIC / Mazer, Joel (speaker) (Rutgers University)
The modification of jet substructure in heavy-ion collisions compared to that in the vacuum reference is one of the main features of jet quenching. Such modification has been observed at LHC kinematics with various observables, such as jet fragmentation and jet shapes. [...]
2020 - 1445. Conferences; 10th International Conference on Hard and Electromagnetic Probes of High-Energy Nuclear Collisions External links: Talk details; Event details In : 10th International Conference on Hard and Electromagnetic Probes of High-Energy Nuclear Collisions

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Jet-hadron correlations measured relative to the second order event plane in Pb-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 2.76 TeV / ALICE Collaboration
The Quark Gluon Plasma (QGP) produced in ultra relativistic heavy-ion collisions at the Large Hadron Collider (LHC) can be studied by measuring the modifications of jets formed by hard scattered partons which interact with the medium. We studied these modifications via angular correlations of jets with charged hadrons for jets with momenta 20 < $p_{\rm{T}}^{\rm{jet}}$ < 40 GeV/$c$ as a function of the associated particle momentum. [...]
arXiv:1910.14398; CERN-EP-2019-244.- Geneva : CERN, 2020-06-04 - 19 p. - Published in : Phys. Rev. C 101 (2020) 064901 Fulltext: 1910.14398 - PDF; CERN-EP-DRAFT-ALICE-2019-035 - draft - PDF; Fulltext from publisher: PDF;

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Jet-hadron correlations relative to the event plane Pb-Pb collisions at the LHC in ALICE / Mazer, Joel Anthony
In relativistic heavy ion collisions at the Large Hadron Collider (LHC), a hot, dense and strongly interacting medium known as the Quark Gluon Plasma (QGP) is produced [...]
CERN-THESIS-2017-372. - 223 p.

Full text - Full text - Full text

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$\phi$ meson production at forward rapidity in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}}=2.76$ TeV / ALICE Collaboration
$\phi$ meson measurements provide insight into strangeness production, which is one of the key observables for the hot medium formed in high-energy heavy-ion collisions. ALICE measured $\phi$ production through its decay in muon pairs in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}}$ = 2.76 TeV in the intermediate transverse momentum range $2 < p_{\rm T} < 5$ GeV/$c$ and in the rapidity interval $2.5<y<4$. [...]
arXiv:1804.08906; CERN-EP-2018-082.- Geneva : CERN, 2018-07-07 - 26 p. - Published in : Eur. Phys. J. C 78 (2018) 559 Article from SCOAP3: PDF; Draft (restricted): PDF; Fulltext: PDF; Fulltext from Publisher: PDF;

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Neutral pion and $\eta$ meson production at mid-rapidity in Pb–Pb collisions at $\sqrt{s_{NN}}=2.76$ TeV / ALICE Collaboration
Neutral pion and η meson production in the transverse momentum range 1 < $p_{T}$ < 20 GeV/$c$ have been measured at mid-rapidity by the ALICE experiment at the Large Hadron Collider (LHC) in central and semi-central Pb-Pb collisions at $\sqrt{s_{NN}}=2.76$ TeV. These results were obtained using the photon conversion method as well as the PHOS and EMCal detectors. [...]
arXiv:1803.05490; CERN-EP-2018-040.- Geneva : CERN, 2018-10-10 - 20 p. - Published in : Phys. Rev. C 98 (2018) 044901 Draft (restricted): PDF; Fulltext: PDF;

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Jet-hadron correlations relative to the event plane at the LHC with ALICE / Mazer, Joel (Tennessee U.) /ALICE
In ultra relativistic heavy-ion collisions at the Large Hadron Collider (LHC), conditions are met to produce a hot, dense and strongly interacting medium known as the Quark Gluon Plasma (QGP). Quarks and gluons from incoming nuclei collide to produce partons at high momenta early in the collisions. [...]
2017 - 4 p. - Published in : Nucl. Phys. A 967 (2017) 500-503 Fulltext: PDF;
In : The XXVI international conference on ultrarelativistic heavy-ion collisions, Chicago, United States Of America, 6 - 11 Feb 2017, pp.500-503

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Neutral pion and $\eta$ meson production in p-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV / ALICE Collaboration
Neutral pion and $\eta$ meson invariant differential yields were measured in non-single diffractive p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV with the ALICE experiment at the CERN LHC. The analysis combines results from three complementary photon measurements, utilizing the PHOS and EMCal calorimeters and the Photon Conversion Method. [...]
arXiv:1801.07051; CERN-EP-2018-002.- Geneva : CERN, 2018-08-06 - 34 p. - Published in : Eur. Phys. J. C 78 (2018) 624 Article from SCOAP3: PDF; Draft (restricted): PDF; Fulltext: PDF;

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10.

$\Lambda_{\rm c}^+$ production in pp collisions at $\sqrt{s} = 7$ TeV and in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV / ALICE Collaboration
The $p_{\rm T}$-differential production cross section of prompt $\Lambda_{\rm c}^+$ charmed baryons was measured with the ALICE detector at the Large Hadron Collider (LHC) in pp collisions at $\sqrt{s} = 7$ TeV and in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV at midrapidity. The $\Lambda_{\rm c}^+$ and ${\overline{\Lambda}}_{\rm c}^-$ were reconstructed in the hadronic decay modes $\Lambda_{\rm c}^+\rightarrow {\rm p}{\rm K^-}\pi^+$, $\Lambda_{\rm c}^+\rightarrow {\rm p}{\rm K_{\rm S}^0}$ and in the semileptonic channel $\Lambda_{\rm c}^+\rightarrow {\rm e^+}\nu_{\rm e}\Lambda$ (and charge conjugates). [...]
arXiv:1712.09581; CERN-EP-2017-339.- Geneva : CERN, 2018-04-18 - 40 p. - Published in : JHEP 04 (2018) 108 Article from SCOAP3: 1645239_scoap3-fulltext - PDF; scoap - PDF; Draft (restricted): PDF; Fulltext: 1645239_arXiv:1712.09581 - PDF; arXiv:1712.09581 - PDF; External links: 00006 Product of acceptance and efficiency for the two \Lc hadronic decay channels in p-Pb collisions at \sqrtsNN = 5.02 \tev, as a function of \pt with the MVA technique. From left to right: \LctopKpi and \LctopKzS. The solid lines correspond to the prompt \Lc, while the dotted lines represent $(A \times \epsilon)$ for the \Lc from beauty-hadron decays. The statistical uncertainties are smaller than the marker size.; 00003 Invariant-mass distribution of $\Lcplus$ candidates (and charge conjugates) for $4 <$ \pt $< 6$ \gevc in \pPb collisions at \sqrtsNN = 5.02~\tev. The dashed lines represent the fit to the background while the solid lines represent the total fit function. Top-left: $\LctopKpi$ STD analysis, top-right: $\LctopKpi$ MVA, bottom-left: $\LctopKzS$ STD analysis and bottom-right: $\LctopKzS$ MVA.; 00005 Product of acceptance and efficiency for \Lc in pp collisions at $\sqrt{s}=7~\TeV$, as a function of \pt. From left to right: \LctopKpi, \LctopKzS, and \LctoenuLambda. For hadronic decays the solid lines correspond to the prompt \Lc, while the dotted lines represent $(A \times \epsilon)$ for \Lc baryons originating from beauty-hadron decays. The efficiency for semi-leptonic decays (same for both prompt and non-prompt \Lc) is represented with one solid line. The statistical uncertainties are smaller than the marker size.

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4	Mazer, J
1	Mazer, J A
12	Mazer, J.
7	Mazer, J.A.
147	Mazer, Joel Anthony

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