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The shear viscosity of a variety of strongly interacting quantum fluids, ranging from ultracold atomic Fermi gases to quark-gluon plasmas, can be accurately measured.
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The value of Φ 0 \Phi_{0} given in Eq. ( 6
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It is numerically convenient to solve Eq. ( 15
Cited in the paper.
This can be seen as follows: ω z ( 1 ) ( r , t ) \omega^{(1)}_{z}(r,t) obeys the 2D equation of motion [ 2 ] ∂ t ω z ( 1 ) ( r , t ) = ν ∇ 𝒓 2 ω z ( 1 ) ( r , t ) \partial_{t}\omega^{(1)}_{z}(r,t)=\nu\nabla^{2}_{\bm{r}}\omega^{(1)}_{z}(r,t) . Therefore, ν \nu plays the role of diffusion constant for ω z ( 1 ) ( r , t ) \omega^{(1)}_{z}(r,t) . This happens because the 2D flow in our case is uniform and incompressible to 𝒪 ( Φ 0 ) {\cal O}(\Phi_{0})
Cited in the paper.