Speaker
Description
Ideally, the Statistical Hadronization Model (SHM) freeze-out curve should reveal the QCD parton-hadron phase transformation line in the ($T$,$μ_B$) plane. We discuss the effects of various final state interaction phenomena, like baryon-antibaryon annihilation, core-corona effects or QCD critical point formation, which shift or deform the SHM freezeout curve. In particular, we present a method to remove the annihilation effects by quantifying them with the microscopic hadron transport model UrQMD[1].
We further discuss the new aspects of hadronization that could be associated with the relatively broad cross-over phase transformation as predicted by lattice-QCD theory at low $μ_{B}$. That opens up the possibility that various observables of hadronization, e.g. hadron formation or susceptibilities of higher order (related to grand canonical fluctuations of conserved hadronic charges) may freeze out at different characteristic temperatures. This puts into question the concept of a universal (pseudo)critical temperature, as does the very nature of a cross-over phase transformation.
[1] F. Becattini, J. Steinheimer, R. Stock and M. Bleicher, Phys.Lett. B764 (2017) 241-246
| Content type | Theory |
|---|---|
| Centralised submission by Collaboration | Presenter name already specified |
