the non-local viscosity were calculated. The longitudinal and transverse non-local charge conductivities as functions of wave-vector $q$ and frequency $\omega$ are given by $$\begin{aligned}
\sigma_{\parallel} & = & \frac{\sigma_{0}}{1-i\tau_{c,1}\omega+i\frac{\tau_{c,1}}{\tau_{V}}\frac{vq}{\omega}+\frac{1}{4}v^{2}\tau_{c,1}q^{2}\left(\frac{2i}{\omega}+\frac{1}{M_{c}\left(q,\omega\right)-i\omega}\right)},\nonumber \\
\sigma_{\bot} & = & \frac{\sigma_{0}}{1-i\tau_{c,1}\omega+\frac{\frac{1}{4}v^{2}\tau_{c,1}q^{2}}{M_{c}\left(q,\omega\right)-i\omega}},\end{aligned}$$ where $\sigma_{0}=\frac{2e^{2}\log\left(2\right)k_{B}T\tau_{c,1}}{\pi\hbar^{2}}$ is the conductivity at vanishing wave-numbers and frequencies [@Fritz2008]. $M_{c}$ is a memory function containing information on scattering in high angular momentum channels $m\geq2$: $$M_{c}\left(q,\omega\right)=\tau_{c,2}^{-1}+\frac{1}{2}vq\frac{\textrm{I}_{3+\frac{\eta_{c}}{\gamma_{c}}-i\omega\tau_{c}}\left(\tau_{c}vq\right)}{\textrm{I}_{2+\frac{\eta_{c}}{\gamma_{c}}-i\omega\tau_{c}}\left(\tau_{c}vq\right)}.\label{eq:memory}$$ This result is a direct consequence of the depence of the scattering rate $\tau_{c,m}^{-1}\sim\alpha^{2}k_{B}T\left|m\right|$ on the angular momentum state of the Dirac electron. A similar $\tau_{c,m}^{-1}\sim\left|m\right|$ was found in Ref.[@Mirlin1997] for scattering off a random magnetic field and gives rise to similar expressions for the nonlocal conductivities, caused by rather different microscopic mechanism. In Eq. (\[eq:memory\]), $\tau_{c}$, $\gamma_{c}$ and $\eta_{c}$ determine the slopes and the offset in Eq. (\[eq:summary\_scattering\_rates\]) (see Sec. \[subsec:Scattering-times\]), $\tau_{V}$ characterizes the strength of long range Coulomb interactions (see Eq. (\[eq:Vlasov\_time\])). The results for the non-local thermal conductivity and viscosity are given in Eqs. (\[eq:thermal\_conductivity\_result\]), and (\[eq:viscosity\_result\]). The transport coefficients show pronounced resonance features at $vq\approx\omega$ where $q$ and $\omega$ are the wavenumber and frequency of the applied electric field or thermal gradient (see Figs. \[fig:Fig\_charge\_conductivities\], \[fig:Fig\_thermal\_conductivities\]) and $v$ is the electron group velocity. The 