In an isotropic chiral active fluid, requiring the total momentum stress to be symmetric leaves only the odd Hall viscosity and an odd pressure as measurable odd coefficients at hydrodynamic times.
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Chiral active fluids: what can we learn from the total momentum?
In an isotropic chiral active fluid, requiring the total momentum stress to be symmetric leaves only the odd Hall viscosity and an odd pressure as measurable odd coefficients at hydrodynamic times.