condensed matter - What's chiral about the Dirac points in graphene?

One of the main interesting properties of graphene is the appearance of Dirac points in its energy band structure, i.e. the presence of points where the valence and conduction bands meet at conical intersections at which the dispersion is (locally) the same as for massless fermions moving at the speed of light.

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These Dirac points occur at the vertices of the standard hexagonal Brillouin zone, and they come in two sets of three, normally denoted $K$ and $K'$. Surprisingly, however, these two sets (despite looking much the same) turn out to be inequivalent: as far as the lattice translations know, the three $K$ points are exactly the same, but there's nothing in the lattice translation symmetry that relates them to the $K'$ points.

Even more interestingly, these two Dirac points are generally referred to as having a specific chirality (as an example, see Phys. Rev. Lett. 107, 166803 (2011)). Now, I understand why the two are not fully equivalent (as a simple insight, if you rotate the lattice by 60° about a carbon, you don't get the same lattice, which you do after 120°) and why they're related by a reflection symmetry (obvious in the diagram above, and also by the fact that if you tag the two inequivalent carbons as in this question, a 60° rotation is equivalent to a reflection on a line); since the two are inequivalent but taken to each other by a mirror symmetry, I understand why the designation as 'chiral' applies.

Nevertheless, I normally associate the word chiral (when restricted to 2D objects) as something that can be used to fix an orientation of the plane, or, in other words, something associated with a direction of rotation of that plane, and this is where my intuitive understanding of these $K$ and $K'$ points stops. So, in short:

• in what way are the $K$ and $K'$ points of graphene associated with an orientation and/or a direction of rotation on the plane, in both the real and the dual lattices?

Similarly, and more physically, what is it about the $K$ and $K'$ points that makes them respond differently to chiral external drivers, such as magnetic fields or circularly polarized light?