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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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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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$\Lambda_{\rm c}^+$ 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 $4 <$ \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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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;

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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;

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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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Measurement of Z$^0$-boson production at large rapidities in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV / ALICE Collaboration
The production of Z$^0$ bosons at large rapidities in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV is reported. Z$^0$ candidates are reconstructed in the dimuon decay channel (${\rm Z}^0 \rightarrow \mu^+\mu^-$), based on muons selected with pseudo-rapidity $-4.0<\eta<-2.5$ and $p_{\rm T}>20$ GeV/$c$. [...]
arXiv:1711.10753; CERN-EP-2017-305.- Geneva : CERN, 2018-05-10 - 12 p. - Published in : Phys. Lett. B 780 (2018) 372-383 Article from SCOAP3: PDF; Draft (restricted): PDF; Fulltext: PDF;

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Longitudinal asymmetry and its effect on pseudorapidity distributions in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV / ALICE Collaboration
First results on the longitudinal asymmetry and its effect on the pseudorapidity distributions in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 2.76 TeV at the Large Hadron Collider are obtained with the ALICE detector. The longitudinal asymmetry arises because of an unequal number of participating nucleons from the two colliding nuclei, and is estimated for each event by measuring the energy in the forward neutron-Zero-Degree-Calorimeters (ZNs). [...]
arXiv:1710.07975; CERN-EP-2017-277.- Geneva : CERN, 2018-06-10 - 13 p. - Published in : Phys. Lett. B 781 (2018) 20-32 Article from SCOAP3: PDF; Fulltext: arXiv:1710.07975 - PDF; CERN-EP-DRAFT-ALICE-2017-026 - draft - draft - draft - PDF;

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10.

Production of $^{4}$He and $^{4}\overline{\textrm{He}}$ in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 2.76 TeV at the LHC / Acharya, Shreyasi (Calcutta, VECC) ; Adamova, Dagmar (Rez, Nucl. Phys. Inst.) ; Adolfsson, Jonatan (Lund U.) ; Aggarwal, Madan Mohan (Panjab U.) ; Aglieri Rinella, Gianluca (CERN) ; Agnello, Michelangelo (Turin Polytechnic) ; Agrawal, Neelima (Indian Inst. Tech., Mumbai) ; Ahammed, Zubayer (Calcutta, VECC) ; Ahn, Sang Un (KISTI, Daejeon) ; Aiola, Salvatore (Yale U.) et al. /ALICE ; ALICE Collaboration
Results on the production of $^{4}{\textrm{He}}$ and $^{4}\overline{\textrm{He}}$ nuclei in Pb-Pb collisions at $ \sqrt{s_{\mathrm{NN}}} = 2.76 $ TeV in the rapidity range $ \mid y \mid < 1$, using the ALICE detector, are presented in this paper. The rapidity densities corresponding to 0-10% central events are found to be $\mathrm{d}N/\mathrm{d}y _{^{4}\mathrm{He}} = (0.8 \pm 0.4 ~(\mathrm{stat}) \pm 0.3~(\mathrm{syst}))\times 10^{-6}$ and $\mathrm{d}N/\mathrm{d}y _{^{4}\mathrm{\overline{He}}} = (1.1 \pm 0.4~(\mathrm{stat}) \pm 0.2~(\mathrm{syst}))\times 10^{-6}$, respectively. [...]
arXiv:1710.07531; CERN-EP-2017-266.- Geneva : CERN, 2018-03 - 20 p. - Published in : Nucl. Phys. A 971 (2018) 1-20 Draft (restricted): PDF; Fulltext: PDF;

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Se også: lignende forfatternavn
26	Chojnacki, M
1	Chojnacki, M J
27	Chojnacki, M.
1	Chojnacki, MJ
2	Chojnacki, Mateusz
1	Chojnacki, Mateusz Jerzy
13	Chojnacki, Mikolaj

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