Second-order spin hydrodynamics is extended with nonlocal memory corrections, adding new acceleration-dependent terms to diffusion, rotational stress, and heat-current equations.
This discrepancy arises from fluid expansion or compr ession and is mathematically expressed as Π = ⟨ˆp⟩ − p ( ǫ, na, Sαβ) = ⟨ˆp⟩l + ⟨ˆp⟩1 + ⟨ˆp⟩2 − p ( ǫ, na, Sαβ)
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Generalized relativistic second-order spin hydrodynamics from Zubarev's non-equilibrium statistical operator
Second-order spin hydrodynamics is extended with nonlocal memory corrections, adding new acceleration-dependent terms to diffusion, rotational stress, and heat-current equations.