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We consider the visco-elastic response of the electronic degrees of freedom in 2D and 3D topological insulators (TI).
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In Riemannian geometry, the torsion tensor T a = d 𝐞 e + ω a b ∧ 𝐞 b T^{a}=d{\bf e}^{e}+{\omega^{a}}_{b}\wedge{\bf e}^{b} is taken to be zero, which determines ω a b {\omega^{a}}_{b} in terms of 𝐞 a {\bf e}^{a}
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