One of the main challenges in nuclear physics is understanding the emergent phenomena of strongly interacting matter governed by quantum chromodynamics (QCD). Heavy-ion collisions conducted at the Large Hadron Collider at CERN and the Relativistic Heavy Ion Collider at BNL create a unique and puzzling state of matter known as quark-gluon plasma (QGP), where quarks and gluons are deconfined. The QGP behaves like a nearly perfect liquid, which is modeled using relativistic hydrodynamics. Recent experiments have shown that the QGP exhibits spin-polarization phenomena, such as the global polarization of Lambda baryons and the spin alignment of vector mesons.
While existing theoretical models, based on the assumption of local thermodynamic equilibrium of spin degrees of freedom, successfully describe the global polarization, they fail to explain other observables, such as the spin alignment. These discrepancies highlight the need to extend conventional hydrodynamic models to include spin effects. This has motivated the development of what is now called relativistic spin hydrodynamics. Developing relativistic spin hydrodynamics is essential for a deeper understanding of the QGP and hadron polarization in heavy-ion collisions. The main objectives of this proposal are (i) the formulation of causal and stable theories of relativistic spin hydrodynamics, (ii) their extensions to the far-from-equilibrium regime, and (iii) Applications of spin hydrodynamics to QGP physics.