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The next-to-leading order weak-coupling shear viscosity of QCD was computed six years ago.
However, these results have never been applied at finite baryon chemical potential $\mu$, even though intermediate-energy heavy ion collisions and merging neutron stars may explore the Quark-Gluon Plasma in a regime with large baryon chemical potentials.
In this talk, I extend the next-to-leading order shear viscosity calculations to finite $\mu$, and show that, while the convergence of the weak-coupling expansion is questionable for achievable plasmas, it is somewhat better at $\mu > T$ than at $\mu=0$.
Oscar Garcia