$\Lambda$ polarization in very high energy heavy ion collisions as a probe of the Quark-Gluon Plasma formation and properties

TL;DR

This study investigates the polarization of $\\Lambda$ hyperons in high-energy heavy ion collisions to probe the Quark-Gluon Plasma's formation and properties, showing how spin measurements relate to initial flow and viscosity.

Contribution

It provides a detailed theoretical calculation of hyperon polarization including feed-down effects, linking polarization components to initial flow and plasma viscosity, and compares results with experimental data.

Findings

Polarization along the global angular momentum is sensitive to initial longitudinal flow.

Longitudinal polarization component is highly sensitive to the plasma's bulk viscosity.

Results agree well with experimental measurements.

Abstract

We have studied the spin polarization of $\Lambda$ hyperons in heavy ion collisions at center-of-mass energies $\sqrt{s_{NN}} = 200$ GeV and $\sqrt{s_{NN}} = 5.02$ TeV carried out at RHIC and LHC colliders. We have calculated the mean spin vector at local thermodynamic equilibrium, including all known first-order terms in the gradients of the thermo-hydrodynamic fields, assuming that the hadronization hypersurface has a uniform temperature. We have also included the feed-down contributions to the polarization of $\Lambda$ stemming from the decays of polarized $\Sigma^*$ and $\Sigma^0$ hyperons. The obtained results are in good agreement with the data. In general, the component of the spin vector along the global angular momentum, orthogonal to the reaction plane, shows strong sensitivity to the initial longitudinal flow velocity. Furthermore, the longitudinal component of the spin vector turns out to be very sensitive to the bulk viscosity of the plasma at the highest LHC energy. Therefore, the azimuthal dependence of spin polarization can effectively constrain the initial hydrodynamic conditions and the transport coefficients of the Quark Gluon Plasma.