Esther Montes Prado

Relative particle yield fluctuations in Pb-Pb collisions at ${\mathbf{\sqrt{s_{\rm NN}}=2.76}}$ TeV

S. Acharya, G. Bíró, Mónika Varga-Kőfaragó, Richard Daniel Majka et autres

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 …

J/$\psi$ elliptic flow in Pb-Pb collisions at $\mathbf{\sqrt{s_{\rm NN}}}$ = 5.02 TeV

S. Acharya, G. Bíró, Mónika Varga-Kőfaragó, Richard Daniel Majka et autres

We report a precise measurement of the J/$\\psi$ elliptic flow in Pb-Pb collisions at $\\sqrt{s_{\\rm NN}} = 5.02$ TeV with the ALICE detector at the LHC. The J/$\\psi$ mesons are reconstructed at mid-rapidity ($|y| < 0.9$) in the dielectron decay channel and …

Measuring K$^0_{\rm S}$K$^{\rm \pm}$ interactions using Pb-Pb collisions at ${\sqrt{s_{\rm NN}}=2.76}$ TeV : arXiv

S. Acharya, Yosuke Watanabe, J. Milošević, Richard Daniel Majka et autres

Linear and non-linear flow mode in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76$ TeV

S. Acharya, Y. Watanabe, J. Milošević, G. Bíró et autres

Production of $Σ(1385)^{±}$ and $Ξ(1530)^{0}$ in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV

J. Zhu, Xiangrong Zhu, A. Zichichi, Alice Zimmermann et autres

Multiplicity-dependent enhancement of strange and multi-strange hadron production in proton-proton collisions at $\sqrt{s} = 7$ TeV

J. Adam, J. Milošević, G. Bíró, E. García-Solis et autres

The yields of strange (${\\rm K}^{0}_{S}$, $\\Lambda$, $\\bar{\\Lambda}$) and multi-strange ($\\Xi^{-}$, $\\bar{\\Xi}^{+}$, $\\Omega^{-}$, $\\bar{\\Omega}^{+}$) hadrons are measured at midrapidity in proton-proton (pp) collisions at $\\sqrt{s}$ = 7 TeV as a function of the charged-particle multiplicity density (${\\rm d}N_{\\rm ch}/{\\rm d}\\eta$).The production rate …

Drift Kinetic Equation Solver for Grid (DKEsG)

A. J. Rubio Montero, Manuel Rodríguez-Pascual, Esther Montes Prado, Rafael Mayo-García

Neoclassical (NC) transport calculations are necessary for the complete simulation cycle of the behavior of plasmas inside both tokamaks and stellarators, which are more complex to be performed on the latest. In addition, due to the fact that the NC transport is …

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