Emergent canonical spin tensor in the chiral symmetric hot QCD

The spin tensor is fundamental to relativistic spin hydrodynamics, but its definition is ambiguous due to the pseudogauge symmetry. We show that this ambiguity can be solved in interacting field theories. We prove that the mean field limit of the Nambu-Jona-Lasinio model with spin-spin interactions is equivalent to non-dissipative spin hydrodynamics with a canonical spin tensor.