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Isospin kaon anomaly and its consequences

Francesco Giacosa, Martin Rohrmoser

Abstract

Isospin symmetry is well fulfilled in the QCD vacuum, as evidenced by small mass differences of isospin partners and suppressed isospin-violating decays. Recently, the NA61/SHINE collaboration reported an unexpectedly large isospin-violating charged-to-neutral kaon ratio in Ar-Sc heavy-ion collisions (HIC).Using a quark recombination approach, we introduce a function of kaon multiplicities that reduces to unity in the isospin-symmetric limit independently of the scattering energy and type of nuclei. Using this quantity, we show that nucleus-nucleus collisions violate isospin sizably (at the $6.4σ$--level), while proton-proton data on kaon multiplicities do not. We predict other isospin-violating enhancements in HIC, such as the proton-to-neutron ratio $p/n \sim 1.2$ and the hyperon ratio $Σ^{+}/Σ^{-}\sim1.4$. Finally, we extend the approach to antiquarks in the initial state, useful for e.g. pion-nucleus scattering reactions.

Isospin kaon anomaly and its consequences

Abstract

Isospin symmetry is well fulfilled in the QCD vacuum, as evidenced by small mass differences of isospin partners and suppressed isospin-violating decays. Recently, the NA61/SHINE collaboration reported an unexpectedly large isospin-violating charged-to-neutral kaon ratio in Ar-Sc heavy-ion collisions (HIC).Using a quark recombination approach, we introduce a function of kaon multiplicities that reduces to unity in the isospin-symmetric limit independently of the scattering energy and type of nuclei. Using this quantity, we show that nucleus-nucleus collisions violate isospin sizably (at the --level), while proton-proton data on kaon multiplicities do not. We predict other isospin-violating enhancements in HIC, such as the proton-to-neutron ratio and the hyperon ratio . Finally, we extend the approach to antiquarks in the initial state, useful for e.g. pion-nucleus scattering reactions.

Paper Structure

This paper contains 16 equations, 3 figures, 2 tables.

Figures (3)

  • Figure 1: Experimental data for $\tilde{R}_K$ of Eq. (\ref{['rkt']}) from proton-proton collisions, together with the weighted average (constant fit) $\tilde{R}_K =1.030\pm0.038$. The dashed line is the isospin-symmetric prediction $\tilde{R}_K = 1$.
  • Figure 2: Experimental data for $\tilde{R}_K$ of Eq. (\ref{['rkt']}) from nucleus-nucleus collisions, together with the weighted average (constant fit) $\tilde{R}_K=1.185\pm0.029$. The dashed line is the isospin-symmetric prediction $\tilde{R}_K = 1$.
  • Figure 3: Experimental data for $R_K$ of Eq. (\ref{['rk1']}) from nucleus-nucleus collisions, together with the weighted average (constant fit) $R_K = 1.152 \pm 0.027$. The dashed line is the isospin-symmetric prediction $R_K = 1$ valid for $Q/A = 1/2$.