Opacity of graphene independent of light frequency and polarization due to the topological charge of the Dirac points

The opacity of graphene is known to be approximately given by the fine-structure constant $\ensuremath{\alpha}$ times $\ensuremath{\pi}$. We point out the fact that the opacity is roughly independent of the frequency and polarization of the light can be attributed to the topological charge of the Dirac points. As a result, one can literally see the topological charge with the naked eye from the opacity of graphene, and moreover it implies that the fine-structure constant is topologically protected. A similar analysis suggests that 3D topological insulator thin films of any thickness also have opacity $\ensuremath{\pi}\ensuremath{\alpha}$ in the infrared region owing to the topological surface states, indicating that one can see the surface states with the naked eye through an infrared lens. For 3D Dirac or Weyl semimetals, the optical absorption power is linear to the frequency in the infrared region, with a linearity given by the fine-structure constant and the topological charge of Weyl points.