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1.
$\phi$ 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;
2.
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;
3.
Azimuthally-differential pion femtoscopy relative to the third harmonic event plane in Pb-Pb collisions at $\mathbf{\sqrt{\textit{s}_{_{\rm NN}}}}$ = 2.76 TeV / ALICE Collaboration
Azimuthally-differential femtoscopic measurements, being sensitive to spatio-temporal characteristics of the source as well as to the collective velocity fields at freeze out, provide very important information on the nature and dynamics of the system evolution. While the HBT radii oscillations relative to the second harmonic event plane measured recently reflect mostly the spatial geometry of the source, model studies have shown that the HBT radii oscillations relative to the third harmonic event plane are predominantly defined by the velocity fields. [...]
arXiv:1803.10594; CERN-EP-2018-035.- Geneva : CERN, 2018-10-10 - 12 p. - Published in : Phys. Lett. B 785 (2018) 320-331 Article from SCOAP3: PDF; Draft (restricted): PDF; Fulltext: PDF;
4.
Transverse momentum spectra and nuclear modification factors of charged particles in pp, p-Pb and Pb-Pb collisions at the LHC / ALICE Collaboration
We report the measured transverse momentum ($p_{\rm T}$) spectra of primary charged particles from pp, p-Pb and Pb-Pb collisions at a center-of-mass energy $\sqrt{s_{\rm NN}} = 5.02$ TeV in the kinematic range of $0.15<p_{\rm T}<50$ GeV/$c$ and $|\eta|< 0.8$. A significant improvement of systematic uncertainties motivated the reanalysis of data in pp and Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV, as well as in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV, which is also presented. [...]
arXiv:1802.09145; CERN-EP-2018-025.- Geneva : CERN, 2018-11-06 - 27 p. - Published in : JHEP 11 (2018) 013 Article from SCOAP3: PDF; Draft (restricted): PDF; Fulltext: PDF;
5.
Prompt and non-prompt J/$\psi$ production and nuclear modification at mid-rapidity in p-Pb collisions at ${\bf \sqrt{{\it s}_{\text{NN}}}= 5.02}$ TeV / ALICE Collaboration
A measurement of beauty hadron production at mid-rapidity in proton-lead collisions at a nucleon-nucleon centre-of-mass energy $\sqrt{s_{\rm NN}}=5.02$ TeV is presented. The semi-inclusive decay channel of beauty hadrons into J/$\psi$ is considered, where the J/$\psi$ mesons are reconstructed in the dielectron decay channel at mid-rapidity down to transverse momenta of 1.3 GeV/$c$. [...]
arXiv:1802.00765; CERN-EP-2018-010.- Geneva : CERN, 2018-06-08 - 24 p. - Published in : Eur. Phys. J. C 78 (2018) 466 Article from SCOAP3: PDF; Draft (restricted): PDF; Fulltext: 1802.00765 - PDF; arXiv:1802.00765 - PDF;
6.
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;
7.
$\Lambda_{\rm c}^+$ 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: scoap - PDF; 1645239_scoap3-fulltext - PDF; Draft (restricted): PDF; Fulltext: arXiv:1712.09581 - PDF; 1645239_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 $4 &lt;$ \pt $&lt; 6$ \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.
8.
First measurement of $\Xi_{\rm c}^0$ production in pp collisions at $\mathbf{\sqrt{s}}$ = 7 TeV / ALICE Collaboration
The production of the charm-strange baryon $\Xi_{\rm c}^0$ is measured for the first time at the LHC via its semileptonic decay into e$^+\Xi^-\nu_{\rm e}$ in pp collisions at $\sqrt{s}=7$ TeV with the ALICE detector. The transverse momentum ($p_{\rm T}$) differential cross section multiplied by the branching ratio is presented in the interval 1 $<$ $p_{\rm T}$ $<$ 8 GeV/$c$ at mid-rapidity, $|y|$ $<$ 0.5. [...]
arXiv:1712.04242; CERN-EP-2017-332.- Geneva : CERN, 2018-06-10 - 12 p. - Published in : Phys. Lett. B 781 (2018) 8-19 Article from SCOAP3: PDF; Draft (restricted): PDF; Fulltext: arXiv:1712.04242 - PDF; S0370269318302570 - XML;
9.
Constraints on jet quenching in p-Pb collisions at $\mathbf{\sqrt{s_{NN}}}$ = 5.02 TeV measured by the event-activity dependence of semi-inclusive hadron-jet distributions / ALICE Collaboration
The ALICE Collaboration reports the measurement of semi-inclusive distributions of charged-particle jets recoiling from a high-transverse momentum trigger hadron in p-Pb collisions at $\sqrt{s_{\rm NN}} =5.02$ TeV. Jets are reconstructed from charged-particle tracks using the anti-$k_{\rm T}$ algorithm with resolution parameter $R=0.2$ and $0.4$. [...]
arXiv:1712.05603; CERN-EP-2017-324.- Geneva : CERN, 2018-08-10 - 19 p. - Published in : Phys. Lett. B 783 (2018) 95-113 Article from SCOAP3: PDF; Draft (restricted): PDF; Fulltext: PDF;
10.
Relative particle yield fluctuations in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV / ALICE Collaboration
First results on K/$\pi$, p/$\pi$ and K/p fluctuations are obtained with the ALICE detector at the CERN LHC as a function of centrality in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76$ TeV. The observable $\nu_{\rm dyn}$, which is defined in terms of the moments of particle multiplicity distributions, is used to quantify the magnitude of dynamical fluctuations of relative particle yields and also provides insight into the correlation between particle pairs. [...]
arXiv:1712.07929; CERN-EP-2017-318.- Geneva : CERN, 2019-03-14 - 19 p. - Published in : Eur. Phys. J. C 79 (2019) 236 Article from SCOAP3: PDF; Draft (restricted): PDF; Fulltext: PDF; Fulltext from Publisher: PDF;

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