# Crystalline topological insulators

## Introduction

Crystalline topological insulators are introduced by Liang Fu from MIT.

## The role of crystalline symmetries

In the very beginning of the course, we told you that conservation laws - unitary symmetries of the Hamiltonian - do not lead to striking consequences on topology. They allow to reduce the problem by making the Hamiltonian block-diagonal, but not much else (see also Shinsei Ryu's introductory video to week eight).

At first sight, it may seem that crystalline symmetries: mirror or reflection symmetries, rotation symmetries, and so on - are no exception to the above consideration. They are unitary symmetries whose operators commute with the Hamiltonian.

Nevertheless, the role of crystalline symmetries can be quite subtle and it can have important . The reason is that crystalline symmetries are non-local. They relate one point in a crystal to another point, possibly a very distant point. This means that in terms of the Bloch Hamiltonian of the crystal, these symmetries mix different values of momentum.

Consider for instance a 2D crystal with a reflection symmetry

Due to this type of constraint on the Brillouin zone, crystalline symmetries can have important consequences on the topological properties of Bloch Hamiltonians.

Note however, that sometimes the mere presence of a surface can break a crystalline symmetry of the bulk, so that one should be careful when applying the bulk-boundary correspondence to properties based on crystalline symmetries.

## Reflection symmetry

The second-simplest crystalline symmetry (after translation symmetry of course) occurring in many materials is reflection (or mirror) symmetry around one spatial coordinate. For instance, in a 3D crystal, reflection symmetry around the

Reflection symmetry also applies a 180 degree rotation about the

Next if we consider the application of reflection symmetry to either a two-dimensional material or plane in a three dimensional material, then we can choose

In this case, the topological classification follows rather simply from our earlier discussion.

If the Hamiltonian overall is trivial then the total Chern number

N++N−=0 so we can classify the 2 dimensional mirror symmetric Hamiltonians by amirror Chern numberNM=N+−N− .

The mirror Chern number is a topological invariant in the sense that it cannot change without a closure of the bulk gap provided the reflection symmetry is held intact. Moreover the reflection symmetry, together with non-trivial values of the invariant will guarantee edge states.

Naturally, the same recipe allows to construct a reflection symmetric topological insulator starting from any other topological invariant, not just a Chern number. We will now try to do this.

## Examples

Let's think, what could be the simplest topological system protected by reflection symmetry.

We need

We can put two nanowires in a unit cell of the lattice and make their parameters different. That way the weak topological invariant is trivial (there is an even number of Majoranas per unit cell).

On the other hand, if the hopping between the nanowires is reflection invariant, there will be a reflection symmetry axis passing through each nanowire, like this:

If we do everything right (this does require some trial and error in searching for the hopping that actually can couple the two Majoranas from the edge), we get a painfully familiar dispersion:

The same way we can also construct a tight-binding model with a mirror Chern number. The only difference with the Majorana wires that we need to worry about is that Chern number is a

This means that the Chern number of the alternating layers has to have opposite signs, or otherwise the surface would just have surface states going in a single direction.

Once again, coupling the layers we get a familiar Dirac cone on the surface:

Of course also now the dispersion of the edge states looks exactly like what we saw already because all the edge state dispersion in any topological insulator is just given by the Dirac equation.

## Experimental realization of a 3D crystalline topological insulator

As mentioned by Liang Fu, three dimensional crystalline topological insulators have been both predicted and also found in nature. The magical material, which is topological turns out to be a material SnTe, which is actually a "rock-salt" structure. We won't bore you with the details of the rock-salt structure, which you can find for yourself on Wikipedia.

We will just start with the key ingredients for the crystalline topological insulator, namely the symmetries of the crystal: the spatial inversion

While the reflection symmetry acts non-trivially on general wave-vectors

Figure copyright of the Zahid Hasan lab, Princeton, 2015, available under CC-BY-NC-SA 4.0 International license.

This surface spectrum is very easy to interpret.

The crystal curface you see here is perpendicular to two mirror planes projected on

The reflection symmetry pins the pairs Dirac cones to the mirror planes, while time reversal symmetry requires that their momenta are opposite. The 90 degree rotation symmetry interchanges the pairs of cones.

## Conclusion

In short, crystalline topological insulators combine the variety of topological phases with the variety of the crystalline symmetry groups, leading to a multitude of new opportunities.