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$J/ψ$ suppression in Pb+Pb collisions and $p_T$ broadening

Physics – Nuclear Physics – Nuclear Theory
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$J/ψ$ suppression in the threshold model and QGP formation time

Physics – Nuclear Physics – Nuclear Theory
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$J/ψ$ suppression in the threshold model at RHIC and LHC energy

Physics – Nuclear Physics – Nuclear Theory
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$J/ψ$-kaon cross section in meson exchange model

Physics – Nuclear Physics – Nuclear Theory
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$J/Ψ$-nuclear bound states

Physics – Nuclear Physics – Nuclear Theory
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$J/ψ$-Nucleon Scattering Length and In-medium Mass Shift of $J/ψ$ in QCD Sum Rule Analysis

Physics – Nuclear Physics – Nuclear Theory
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$J/ψ\rightarrow p\bar{p}φ$ decay in the isobar resonance model

Physics – Nuclear Physics – Nuclear Theory
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$K/π$, $K/p$ and $p/π$ Ratio Fluctuations within the HSD Transport Approach

Physics – Nuclear Physics – Nuclear Theory
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$K^- p \rightarrow ηΛ$ reaction in an effective Lagrangian model

Physics – Nuclear Physics – Nuclear Theory
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$K^-$ - nucleus relativistic mean field potentials consistent with kaonic atoms

Physics – Nuclear Physics – Nuclear Theory
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$K^-$ and $\bar p$ deeply bound atomic states

Physics – Nuclear Physics – Nuclear Theory
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$K^-$ and $\bar p$ Spectra for Au+Au Collisions at $\sqrt{s}$ = 200 GeV from STAR, PHENIX and BRAHMS in Comparison to Core-Corona Model Predictions

Physics – Nuclear Physics – Nuclear Theory
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$K^-$-Nucleus Scattering at Low and Intermediate Energies

Physics – Nuclear Physics – Nuclear Theory
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$K^-/K^+$ ratio in heavy-ion collisions at GSI with an antikaon self-energy in hot and dense matter

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$K^-/K^+$ ratios in relativistic heavy-ion collisions

Physics – Nuclear Physics – Nuclear Theory
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$K^-pp$ system with chiral SU(3) effective interaction

Physics – Nuclear Physics – Nuclear Theory
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$K^{*0}$ and $Σ^*$ production in Au+Au collisions at $\sqrt{s_{NN}}=$ 200 GeV and 62.4 GeV

Physics – Nuclear Physics – Nuclear Theory
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$K^{*}(892)$ Production in Au+Au and pp Collisions at $\sqrt{s_{NN}}$ = 200GeV at STAR

Physics – Nuclear Physics – Nuclear Experiment
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$K^{+}$ and $K^{-}$ potentials in hadronic matter can be observed

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$K^{\ast}(892)^0$ and $\bar{K}^{\ast}(892)^0$ production in central Pb+Pb, Si+Si, C+C and inelastic p+p collisions at 158$A$~GeV

Physics – Nuclear Physics – Nuclear Experiment
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